TECHNICAL FIELD
[0001] The present invention relates to an inspection system, an inspection method, and
a program, and is suitably used for inspecting a track of a railway vehicle, in particular.
The present application is based upon and claims the benefit of priority of the prior
Japanese Patent Application No. 2018-230834, filed in Japan on December 10, 2018, the entire contents of which are incorporated
herein by reference.
BACKGROUND ART
[0002] When a railway vehicle travels on a track, a position of the track changes due to
a load from the railway vehicle. When such a change in track occurs, there is a possibility
that the railway vehicle exhibits abnormal behavior. Accordingly, Patent Literature
1 discloses a technique in which angular displacements of wheel sets in a yawing direction,
state variables derived by a filter that performs data assimilation, and a measured
value of a forward-and-backward-direction force being a force in a forward and backward
direction that occurs in a member for supporting an axle box are substituted into
motion equations that describe yawings of the wheel sets to derive track irregularity
(alignment irregularity amount and the like) of a railway vehicle.
CITATION LIST
PATENT LITERATURE
SUMMARY OF INVENTION
TECHNICAL PROBLEM
[0004] However, in the technique described in Patent Literature 1, the measured value of
the forward-and-backward-direction force and measured values of accelerations of the
wheel set and a bogie (and a vehicle body in addition to the above, according to need),
respectively, in a right and left direction are used when performing the data assimilation.
These measured values can be obtained without using special sensors, but the number
of sensors disposed in the railway vehicle is preferably as small as possible.
[0005] The present invention has been made in view of the problems as described above, and
an object thereof is to reduce the number of sensors which are used for detecting
track irregularity of a railway vehicle.
SOLUTION TO PROBLEM
[0006] An inspection system of the present invention includes: a data acquisition means
that acquires data of a measured value of a forward-and-backward-direction force as
data of a measured value to be measured by causing a railway vehicle including a vehicle
body, a bogie, and a wheel set to travel on a track; a state variable derivation means
that derives state variables being variables to be determined in a state equation
constituted by using motion equations that describe motions of the railway vehicle,
by using the measured value of the forward-and-backward-direction force; and a track
state derivation means that derives information reflecting a state of the track, in
which the forward-and-backward-direction force is a force in a forward and backward
direction that occurs in a member disposed between the wheel set and the bogie on
which the wheel set is provided, and is a force to be determined according to a difference
between an angular displacement of the wheel set in a yawing direction and an angular
displacement of the bogie on which the wheel set is provided in the yawing direction,
the member is a member for supporting an axle box, the forward and backward direction
is a direction along a traveling direction of the railway vehicle, the yawing direction
is a pivoting direction with an up and down direction being a direction vertical to
the track set as a pivot axis, the state equation is an equation described by using
the state variables, the forward-and-backward-direction force, and a transformation
variable, the state variables include a displacement and a velocity of the bogie in
a right and left direction, an angular displacement and an angular velocity of the
bogie in the yawing direction, an angular displacement and an angular velocity of
the bogie in a rolling direction, a displacement and a velocity of the wheel set in
the right and left direction, and an angular displacement of an air spring attached
to the railway vehicle in the rolling direction, and do not include an angular displacement
and an angular velocity of the wheel set in the yawing direction, the rolling direction
is a pivoting direction with the forward and backward direction set as a pivot axis,
the transformation variable is a variable that performs mutual transformation between
the angular displacement of the wheel set in the yawing direction and the angular
displacement of the bogie in the yawing direction, the track state derivation means
uses the angular displacement of the bogie in the yawing direction, which is one of
the state variables derived by the state variable derivation means, and an actual
value of the transformation variable to derive an estimated value of the angular displacement
of the wheel set in the yawing direction, and uses the derived estimated value of
the angular displacement of the wheel set in the yawing direction to derive the information
reflecting the state of the track, the actual value of the transformation variable
is derived by using the measured value of the forward-and-backward-direction force,
and the state variable derivation means derives the state variables without using
measured values of accelerations of the bogie, the wheel set, and the vehicle body
in the right and left direction during a period in which the measured value of the
forward-and-backward-direction force has been obtained.
[0007] An inspection method of the present invention includes: a data acquisition step of
acquiring data of a measured value of a forward-and-backward-direction force as data
of a measured value to be measured by causing a railway vehicle including a vehicle
body, a bogie, and a wheel set to travel on a track; a state variable derivation step
of deriving state variables being variables to be determined in a state equation constituted
by using motion equations that describe motions of the railway vehicle, by using the
measured value of the forward-and-backward-direction force; and a track state derivation
step of deriving information reflecting a state of the track, in which the forward-and-backward-direction
force is a force in a forward and backward direction that occurs in a member disposed
between the wheel set and the bogie on which the wheel set is provided, and is a force
to be determined according to a difference between an angular displacement of the
wheel set in a yawing direction and an angular displacement of the bogie on which
the wheel set is provided in the yawing direction, the member is a member for supporting
an axle box, the forward and backward direction is a direction along a traveling direction
of the railway vehicle, the yawing direction is a pivoting direction with an up and
down direction being a direction vertical to the track set as a pivot axis, the state
equation is an equation described by using the state variables, the forward-and-backward-direction
force, and a transformation variable, the state variables include a displacement and
a velocity of the bogie in a right and left direction, an angular displacement and
an angular velocity of the bogie in the yawing direction, an angular displacement
and an angular velocity of the bogie in a rolling direction, a displacement and a
velocity of the wheel set in the right and left direction, and an angular displacement
of an air spring attached to the railway vehicle in the rolling direction, and do
not include an angular displacement and an angular velocity of the wheel set in the
yawing direction, the rolling direction is a pivoting direction with the forward and
backward direction set as a pivot axis, the transformation variable is a variable
that performs mutual transformation between the angular displacement of the wheel
set in the yawing direction and the angular displacement of the bogie in the yawing
direction, the track state derivation step uses the angular displacement of the bogie
in the yawing direction, which is one of the state variables derived by the state
variable derivation step, and an actual value of the transformation variable to derive
an estimated value of the angular displacement of the wheel set in the yawing direction,
and uses the derived estimated value of the angular displacement of the wheel set
in the yawing direction to derive the information reflecting the state of the track,
the actual value of the transformation variable is derived by using the measured value
of the forward-and-backward-direction force, and the state variable derivation step
derives the state variables without using measured values of accelerations of the
bogie, the wheel set, and the vehicle body in the right and left direction during
a period in which the measured value of the forward-and-backward-direction force has
been obtained.
[0008] A program of the present invention causes a computer to execute: a data acquisition
step of acquiring data of a measured value of a forward-and-backward-direction force
as data of a measured value to be measured by causing a railway vehicle including
a vehicle body, a bogie, and a wheel set to travel on a track; a state variable derivation
step of deriving state variables being variables to be determined in a state equation
constituted by using motion equations that describe motions of the railway vehicle,
by using the measured value of the forward-and-backward-direction force; and a track
state derivation step of deriving information reflecting a state of the track, in
which the forward-and-backward-direction force is a force in a forward and backward
direction that occurs in a member disposed between the wheel set and the bogie on
which the wheel set is provided, and is a force to be determined according to a difference
between an angular displacement of the wheel set in a yawing direction and an angular
displacement of the bogie on which the wheel set is provided in the yawing direction,
the member is a member for supporting an axle box, the forward and backward direction
is a direction along a traveling direction of the railway vehicle, the yawing direction
is a pivoting direction with an up and down direction being a direction vertical to
the track set as a pivot axis, the state equation is an equation described by using
the state variables, the forward-and-backward-direction force, and a transformation
variable, the state variables include a displacement and a velocity of the bogie in
a right and left direction, an angular displacement and an angular velocity of the
bogie in the yawing direction, an angular displacement and an angular velocity of
the bogie in a rolling direction, a displacement and a velocity of the wheel set in
the right and left direction, and an angular displacement of an air spring attached
to the railway vehicle in the rolling direction, and do not include an angular displacement
and an angular velocity of the wheel set in the yawing direction, the rolling direction
is a pivoting direction with the forward and backward direction set as a pivot axis,
the transformation variable is a variable that performs mutual transformation between
the angular displacement of the wheel set in the yawing direction and the angular
displacement of the bogie in the yawing direction, the track state derivation step
uses the angular displacement of the bogie in the yawing direction, which is one of
the state variables derived by the state variable derivation step, and an actual value
of the transformation variable to derive an estimated value of the angular displacement
of the wheel set in the yawing direction, and uses the derived estimated value of
the angular displacement of the wheel set in the yawing direction to derive the information
reflecting the state of the track, the actual value of the transformation variable
is derived by using the measured value of the forward-and-backward-direction force,
and the state variable derivation step derives the state variables without using measured
values of accelerations of the bogie, the wheel set, and the vehicle body in the right
and left direction during a period in which the measured value of the forward-and-backward-direction
force has been obtained.
BRIEF DESCRIPTION OF DRAWINGS
[0009]
[Fig. 1] Fig. 1 is a view illustrating one example of an outline of a railway vehicle.
[Fig. 2] Fig. 2 is a view conceptually illustrating directions of main motions of
components of the railway vehicle.
[Fig. 3] Fig. 3 is a view illustrating a measured value and a calculated value of
each of acceleration of a bogie in a right and left direction and accelerations of
wheel sets in the right and left direction.
[Fig. 4A] Fig. 4A is a view illustrating one example of an alignment irregularity
amount in a linear track.
[Fig. 4B] Fig. 4B is a view illustrating one example of an alignment irregularity
amount in a curved track.
[Fig. 5] Fig. 5 is a view illustrating one example of a functional configuration of
an inspection apparatus.
[Fig. 6] Fig. 6 is a view illustrating one example of a hardware configuration of
the inspection apparatus.
[Fig. 7] Fig. 7 is a flowchart illustrating one example of processing in the inspection
apparatus.
[Fig. 8] Fig. 8 is a view illustrating one example of a distribution of eigenvalues
of an autocorrelation matrix.
[Fig. 9] Fig. 9 is a view illustrating one example of time-series data of measured
values of forward-and-backward-direction forces (measured values) and time-series
data of predicted values of the forward-and-backward-direction forces (calculated
values).
[Fig. 10] Fig. 10 is a view illustrating one example of time-series data of high-frequency
components of the forward-and-backward-direction forces.
[Fig. 11] Fig. 11 is a view illustrating one example of a configuration of an inspection
system.
[Fig. 12] Fig. 12 is a view illustrating a calculation example, and is a view illustrating
a curvature 1/R of a track being a target of deriving an alignment irregularity amount
and a traveling velocity of the railway vehicle.
[Fig. 13A] Fig. 13A is a view illustrating a calculation example, and is a view illustrating
a first example of a distribution of eigenvalues of an autocorrelation matrix R.
[Fig. 13B] Fig. 13B is a view illustrating a calculation example, and is a view illustrating
a second example of a distribution of eigenvalues of the autocorrelation matrix R.
[Fig. 14] Fig. 14 is a view illustrating a calculation example, and is a view illustrating
time-series data of measured values of forward-and-backward-direction forces and time-series
data of predicted values of the forward-and-backward-direction forces.
[Fig. 15] Fig. 15 is a view illustrating a calculation example, and is a view illustrating
time-series data of high-frequency components of the forward-and-backward-direction
forces.
[Fig. 16A] Fig. 16A is a view illustrating a calculation example based on a method
of a first embodiment, and is a view illustrating a first example of an alignment
irregularity amount yR.
[Fig. 16B] Fig. 16B is a view illustrating a calculation example based on the method
of the first embodiment, and is a view illustrating a second example of the alignment
irregularity amount yR.
[Fig. 17A] Fig. 17A is a view illustrating a calculation example based on a method
of a second embodiment, and is a view illustrating a first example of the alignment
irregularity amount yR.
[Fig. 17B] Fig. 17B is a view illustrating a calculation example based on the method
of the second embodiment, and is a view illustrating the first example of the alignment
irregularity amount yR.
DESCRIPTION OF EMBODIMENTS
[0010] Hereinafter, embodiments of the present invention will be explained while referring
to the drawings.
(Conception)
[0011] First, there will be explained a conception obtained by the present inventors when
realizing embodiments of the present invention.
[0012] Fig. 1 is a view illustrating one example of an outline of a railway vehicle. Note
that in Fig. 1, the railway vehicle is set to proceed in the positive direction of
the x axis (the x axis is an axis along a traveling direction of the railway vehicle).
Further, the z axis is set to a direction vertical to a track 16 (the ground) (a height
direction of the railway vehicle). The y axis is set to a horizontal direction vertical
to the traveling direction of the railway vehicle (a direction vertical to both the
traveling direction and the height direction of the railway vehicle). Further, the
railway vehicle is set to a commercial vehicle. Note that in the respective drawings,
the mark of ● added inside ○ indicates the direction from the far side of the sheet
toward the near side, and the mark of × added inside ○ indicates the direction from
the near side of the sheet toward the far side.
[0013] As illustrated in Fig. 1, in the present embodiment, the railway vehicle includes
a vehicle body 11, bogies 12a, 12b, and wheel sets 13a to 13d. As described above,
in the present embodiment, the railway vehicle including the single vehicle body 11
provided with the two bogies 12a, 12b and four sets of the wheel sets 13a to 13d will
be explained as an example. The wheel sets 13a to 13d have axles 15a to 15d and wheels
14a to 14d provided on both ends of the axles 15a to 15d respectively. In the present
embodiment, a case where each of the bogies 12a, 12b is a bolsterless bogie will be
explained as an example. Note that in Fig. 1, for convenience of illustration, only
the wheels 14a to 14d on one side of the wheel sets 13a to 13d are illustrated, but
wheels are also provided on the other side of the wheel sets 13a to 13d (in the example
illustrated in Fig. 1, there are eight wheels in total). Further, the railway vehicle
includes components other than the components illustrated in Fig. 1 (components and
so on to be explained in later-described motion equations), but for convenience of
illustration, illustrations of these components are omitted in Fig. 1. For example,
the bogies 12a, 12b have bogie frames, bolster springs, and so on. Further, an axle
box is disposed on both sides of each of the wheel sets 13a to 13d in the direction
along the y axis. Further, the bogie frame and the axle box are coupled to each other
by an axle box suspension. The axle box suspension is a device (suspension) to be
disposed between the axle box and the bogie frame. The axle box suspension absorbs
vibration to be transmitted to the railway vehicle from the track 16. Further, the
axle box suspension supports the axle box in a state where the position of the axle
box relative to the bogie frame is restricted, so as to prevent the axle box from
moving in a direction along the x axis and a direction along the y axis relative to
the bogie frame (so as to prevent these movements from occurring preferably). The
axle box suspension is disposed on the both sides of each of the wheel sets 13a to
13d in the direction along the y axis. Note that the railway vehicle itself can be
fabricated by a well-known technique, and thus its detailed explanation is omitted
here.
[0014] When the railway vehicle travels on the track 16, acting force (creep force) between
the wheels 14a to 14d and the track 16 becomes a vibration source and the vibration
sequentially propagates to the wheel sets 13a to 13d, the bogies 12a, 12b, and the
vehicle body 11. Fig. 2 is a view conceptually illustrating directions of main motions
of the components (the wheel sets 13a to 13d, the bogies 12a, 12b, and the vehicle
body 11) of the railway vehicle. The x axis, the y axis, and the z axis illustrated
in Fig. 2 correspond to the x axis, the y axis, and the z axis illustrated in Fig.
1 respectively.
[0015] As illustrated in Fig. 2, in the present embodiment, a case where the wheel sets
13a to 13d, the bogies 12a, 12b, and the vehicle body 11 perform pivoting motion about
the x axis as a pivot axis, pivoting motion about the z axis as a pivot axis, and
motion in the direction along the y axis, will be explained as an example. In the
following explanation, the pivoting motion about the x axis as a pivot axis is referred
to as rolling as necessary, the pivoting direction about the x axis as a pivot axis
is referred to as a rolling direction as necessary, and the direction along the x
axis is referred to as the forward and backward direction as necessary. Note that
the forward and backward direction is the traveling direction of the railway vehicle.
In the present embodiment, the direction along the x axis is set to the traveling
direction of the railway vehicle. Further, the pivoting motion about the z axis as
a pivot axis is referred to as yawing as necessary, the pivoting direction about the
z axis as a pivot axis is referred to as a yawing direction as necessary, and the
direction along the z axis is referred to as the up and down direction as necessary.
Note that the up and down direction is a direction vertical to the track 16. Further,
the motion in the direction along the y axis is referred to as a transversal vibration
as necessary, and the direction along the y axis is referred to as the right and left
direction as necessary. Note that the right and left direction is a direction vertical
to both the forward and backward direction (the traveling direction of the railway
vehicle) and the up and down direction (the direction vertical to the track 16). Further,
the railway vehicle performs motions other than these, but in each of the embodiments,
these motions are not considered in order to simplify the explanation. However, these
motions may be considered.
(First conception)
[0016] In the technique described in Patent Literature 1, the state variables are derived
by performing filtering with a filter (Kalman filter) that performs data assimilation
by using, as observation variables, accelerations y
w1 • •, y
w2 • •, y
w3 • •, y
w4 • • of the wheel sets 13a, 13b, 13c, 13d in the right and left direction, accelerations
y
t1 • •, y
t2 • • of the bogies 12a, 12b in the right and left direction, and in addition to the
above, acceleration y
b • • of the vehicle body 11 in the right and left direction according to need.
[0017] Fig. 3 illustrates a measured value and a calculated value of each of the acceleration
y
t1 • • of the bogie 12a in the right and left direction and the accelerations y
w1 • •, y
w2 • • of the wheel sets 13a, 13b in the right and left direction. The calculated value
is an estimated value of the observation variable calculated by data assimilation.
The horizontal axis in Fig. 3 indicates an elapsed time (second) from a reference
time when the reference time is set to 0 (zero). Concretely, the horizontal axis in
Fig. 3 indicates a measuring time and a calculating time of the acceleration y
t1 • • of the bogie 12a in the right and left direction and the accelerations y
w1 • •, y
w2 • • of the wheel sets 13a, 13b in the right and left direction. When performing the
data assimilation, the estimated value of the state variable is derived so that an
error between a value which is normally given as the measured value of the observation
variable and the estimated value of the observation variable becomes minimum or an
expected value of this error becomes minimum.
[0018] As illustrated in Fig. 3, the measured values of the accelerations y
w1 • •, y
w2• • of the wheel sets 13a, 13b in the right and left direction, and the measured values
of the accelerations y
t1 • •, y
t2 • • of the bogie 12a in the right and left direction include a lot of noises. Based
on this, the present inventors obtained a finding that, depending on a state of the
track 16 (rail), the estimated value does not approximate the measured value and becomes
substantially a fixed value even if the data assimilation is performed. The same applies
to the accelerations y
w3 • •, y
w4 • • of the wheel sets 13c, 13d in the right and left direction, the acceleration
y
t2 • • of the bogie 12b in the right and left direction, and the acceleration y
b • • of the vehicle body 11 in the right and left direction. From the above, the present
inventors considered that there may be a chance that, when deriving the state variables,
the alignment irregularity amounts y
R1, y
R2, y
R3, y
R4 can be derived without greatly decreasing accuracy, even if the measured values of
these accelerations are not used.
[Second conception]
[0019] As described in Patent Literature 1, the present inventors devised a method of calculating
an alignment irregularity amount by using a measured value of force in the forward
and backward direction that occurs in a member disposed between the wheel sets 13a,
13b (13c, 13d) and the bogie 12a (12b) on which these wheel sets 13a, 13b (13c, 13d)
are provided. In the following explanation, the force in the forward and backward
direction that occurs in the member is referred to as a forward-and-backward-direction
force as necessary.
[0020] The alignment irregularity amount is calculated by using an equation representing
a relation between the alignment irregularity amount and the forward-and-backward-direction
force, which is an equation based on a motion equation describing motion when the
railway vehicle travels on a linear track. The track 16 includes a linear portion
and a curved portion. In the following explanation, the linear portion of the track
16 is referred to as a linear track as necessary and the curved portion of the track
16 is referred to as a curved track as necessary.
[0021] When a state equation is constituted by using a motion equation that describes motion
of the railway vehicle traveling on the curved track in the case of performing filtering
with a filter (Kalman filter) performing data assimilation, state variables may diverge.
Therefore, the state equation in the case of performing filtering with the filter
(Kalman filter) that performs data assimilation is constituted by using a motion equation
that describes motion of the railway vehicle traveling on the linear track.
[0022] It is necessary to consider centrifugal force or the like that the railway vehicle
receives when traveling in the motion equation describing the motion of the railway
vehicle traveling on the curved track. Accordingly, the motion equation describing
the motion of the railway vehicle traveling on the curved track includes a term including
a curvature radius of the rail. Therefore, when the state variables are derived by
using the filter (Kalman filter) that performs data assimilation constituted by using
the motion equation that describes the motion of the railway vehicle traveling on
the linear track when the railway vehicle is traveling on the curved track, there
is a risk that it becomes impossible to derive the state variables with high accuracy.
[0023] The present inventors focused attention on the fact that the measured value of the
forward-and-backward-direction force when the railway vehicle travels on the curved
track has a certain bias relative to that when traveling on the linear track. The
component itself of the forward-and-backward-direction force due to the alignment
irregularity occurs in the same manner even on the curved track or the linear track.
Accordingly, the present inventors thought that the alignment irregularity amount
itself has nothing to do with the amount of the aforementioned bias, and thought that
by reducing a low-frequency component (behavior of the aforementioned bias) from time-series
data of the measured value of the forward-and-backward-direction force, the low-frequency
component due to the railway vehicle traveling on the curved track can be reduced
from an estimated value of the state variable even if the filter (Kalman filter) performing
the data assimilation is constituted by using an equation based on the motion equation
that describes the motion of the railway vehicle when traveling on the linear track.
From this, the present inventors devised calculating the alignment irregularity amount
by using the time-series data of the value of the forward-and-backward-direction force
from which the low-frequency component has been reduced. The alignment irregularity
amount is calculated as above, thereby making it possible to calculate the alignment
irregularity amount in the curved track regardless of using the equation based on
the motion equation describing the motion of the railway vehicle when traveling on
the linear track. Further, the calculating equation of the alignment irregularity
amount results in the same calculating equation even on the curved track or the linear
track. Note that there is a chance that even a track, which is designed as a linear
track, actually has a curvature which may exert an influence on estimation accuracy
of the alignment irregularity amount. Therefore, the reduction in the low-frequency
component (behavior of the aforementioned bias) from the time-series data of the measured
value of the forward-and-backward-direction force contributes to improvement of the
estimation accuracy of the alignment irregularity amount on not only the curved track
but also the linear track. Hereinafter, explanation will be made by setting that even
a track, which is designed as a linear track but actually has a curvature which may
exert an influence on estimation accuracy of the alignment irregularity amount, is
also regarded as a curved track.
(Motion equation)
[0024] Next, there will be explained one example of a motion equation that describes the
motion of the railway vehicle. In the present embodiment, there will be explained,
as an example, a case where the railway vehicle has 21 degrees of freedom while taking
the motion equations described in Patent Literature 1 as an example. That is, it is
set that the wheel sets 13a to 13d perform the motion in the right and left direction
(transversal vibration) and the motion in the yawing direction (yawing) (2 × 4 sets
= eight degrees of freedom). Further, it is set that the bogies 12a, 12b perform the
motion in the right and left direction (transversal vibration), the motion in the
yawing direction (yawing), and the motion in the rolling direction (rolling) (3 ×
2 sets = six degrees of freedom). Further, it is set that the vehicle body 11 performs
the motion in the right and left direction (transversal vibration), the motion in
the yawing direction (yawing), and the motion in the rolling direction (rolling) (3
× 1 sets = three degrees of freedom). Further, it is set that air springs (bolster
springs) each provided on the bogies 12a, 12b perform the motion in the rolling direction
(rolling) (1 × 2 sets = two degrees of freedom). Further, it is set that yaw dampers
each provided on the bogies 12a, 12b perform the motion in the yawing direction (yawing)
(1 × 2 sets = two degrees of freedom).
[0025] Note that the degree of freedom is not limited to 21 degrees of freedom. When the
degree of freedom increases, calculation accuracy improves, but a calculation load
becomes high. Further, there is a risk that a later-described Kalman filter no longer
operates stably. It is possible to appropriately determine the degree of freedom by
taking these points into consideration. Further, the following motion equations can
be achieved by representing actions in the respective directions (the right and left
direction, the yawing direction, and the rolling direction) of the respective components
(the vehicle body 11, the bogies 12a, 12b, and the wheel sets 13a to 13d) based on
the descriptions of Non-Patent Literatures 1, 2, for example. Therefore, outlines
of the respective motion equations will be explained here, and their detailed explanations
are omitted. Note that in each of the following equations, there is no term including
the curvature radius (curvature) of the track 16 (rail). That is, each of the following
equations is an equation expressing the railway vehicle traveling on the linear track.
The equation expressing the railway vehicle traveling on the linear track can be obtained
by setting the curvature radius of the track 16 (rail) to be infinite (the curvature
to 0 (zero)) in the equation expressing the railway vehicle traveling on the curved
track.
[0026] In each of the following equations, each subscript w indicates the wheel sets 13a
to 13d. Variables to which (only) the subscript w is added indicate that they are
common to the wheel sets 13a to 13d. Subscripts w1, w2, w3, w4 indicate the wheel
sets 13a, 13b, 13c, 13d respectively.
[0027] Subscripts t, T indicate the bogies 12a, 12b. Variables to which (only) the subscripts
t, T are added indicate that they are common to the bogies 12a, 12b. Subscripts t1,
t2 indicate the bogies 12a, 12b respectively.
[0028] Subscripts b, B indicate the vehicle body 11.
[0029] A subscript x indicates the forward and backward direction or the rolling direction,
a subscript y indicates the right and left direction, and a subscript z indicates
the up and down direction or the yawing direction.
[0030] Further, " • • " and "•" each added above a variable indicate a second-order time
differential and a first-order time differential respectively.
[0031] Note that when the following motion equations are explained, explanations of the
already-explained variables are omitted as necessary. Further, the motion equations
themselves are the same as those described in Patent Literature 1.
[Transversal vibration of wheel set]
[0033] m
w is the mass of the wheel sets 13a to 13d. y
w1 • • is acceleration of the wheel set 13a in the right and left direction (in the
equation, • • is added above y
w1 (the same applies to the other variables below)). f
2 is a lateral creep coefficient (note that the lateral creep coefficient f
2 may be given for each of the wheel sets 13a to 13d). v is a traveling velocity of
the railway vehicle. y
w1 • is a velocity of the wheel set 13a in the right and left direction (in the equation,
• is added above y
w1 (the same applies to the other variables below)). C
wy is a damping constant of the axle box suspension coupling the axle box and the wheel
set in the right and left direction. y
t1 • is a velocity of the bogie 12a in the right and left direction. a represents 1/2
of each distance between the wheel sets 13a and 13b and between the wheel sets 13c
and 13d in the forward and backward direction, which are provided on the bogies 12a,
12b (the distance between the wheel sets 13a and 13b and the distance between the
wheel sets 13c and 13d, which are provided on the bogies 12a, 12b, each become 2a).
φt1 • is an angular velocity of the bogie 12a in the yawing direction. h
1 is a distance between the center of the axle and the center of gravity of the bogie
12a in the up and down direction.
φt1 • is an angular velocity of the bogie 12a in the rolling direction.
φw1 is a pivot amount (angular displacement) of the wheel set 13a in the yawing direction.
K
wy is a spring constant of the axle box suspension in the right and left direction.
y
w1 is a displacement of the wheel set 13a in the right and left direction. y
t1 is a displacement of the bogie 12a in the right and left direction.
φt1 is a pivot amount (angular displacement) of the bogie 12a in the yawing direction.
φt1 is a pivot amount (angular displacement) of the bogie 12a in the rolling direction.
Note that respective variables in (2) Equation to (4) Equation are represented by
being replaced with the variables in (1) Equation according to the meanings of the
subscripts described above.
[Yawing of wheel set]
[0035] I
wz is a moment of inertia of the wheel sets 13a to 13d in the yawing direction.
φw1 • • is angular acceleration of the wheel set 13a in the yawing direction. f
1 is a longitudinal creep coefficient. b is a distance in the right and left direction
between contacts between the two wheels, which are attached to each of the wheel sets
13a to 13d, and the track 16 (rail).
φw1 • is an angular velocity of the wheel set 13a in the yawing direction. C
wx is a damping constant of the axle box suspension in the forward and backward direction.
b
1 represents the length of 1/2 of the interval between the axle box suspensions in
the right and left direction (the interval of the two axle box suspensions, which
are provided on the right and left sides of the single wheel set, in the right and
left direction becomes 2b
1).
γ is a tread slope. r is a radius of the wheels 14a to 14d. y
R1 is an alignment irregularity amount at the position of the wheel set 13a. s
a is an offset from the center of the axles 15a to 15d to an axle box suspension spring
in the forward and backward direction. y
t1 is a displacement of the bogie 12a in the right and left direction. Kwx is a spring
constant of the axle box suspension in the forward and backward direction. Note that
respective variables in (6) Equation to (8) Equation are represented by being replaced
with the variables in (5) Equation according to the meanings of the subscripts described
above. However, y
R2, y
R3, y
R4 are alignment irregularity amounts at the positions of the wheel sets 13b, 13c, 13d
respectively.
[0036] Here, the alignment irregularity is a lateral displacement of a rail in a longitudinal
direction as described in Japan Industrial Standard (JIS E 1001: 2001). The alignment
irregularity amount is an amount of the displacement. Fig. 4A and Fig. 4B each illustrate
one example of the alignment irregularity amount y
R1 at the position of the wheel set 13a. In Fig. 4A, the case of the track 16 being
the linear track will be explained as an example. In Fig. 4B, the case of the track
16 being the curved track will be explained as an example. In Fig. 4A and Fig. 4B,
16a denotes a rail and 16b denotes a crosstie. In Fig. 4A, it is set that the wheel
14a of the wheel set 13a is in contact with the rail 16a at a position 401. In Fig.
4B, it is set that the wheel 14a of the wheel set 13a is in contact with the rail
16a at a position 402. The alignment irregularity amount y
R1 at the position of the wheel set 13a is a distance in the right and left direction
between the contact position between the wheel 14a of the wheel set 13a and the rail
16a and the position of the rail 16a in the case where this position is assumed as
a regular state. The position of the wheel set 13a is the contact position between
the wheel 14a of the wheel set 13a and the rail 16a. The alignment irregularity amounts
y
R2, y
R3, y
R4 at the positions of the wheel sets 13b, 13c, 13d are also defined in the same manner
as the alignment irregularity amount y
R1 at the position of the wheel set 13a.
[Transversal vibration of bogie]
[0037] The motion equations that describe the transversal vibrations of the bogies 12a,
12b (motion in the right and left direction) are expressed by (9) Equation and (10)
Equation below.
[Mathematical equation 3]

[0038] m
T is the mass of the bogies 12a, 12b. y
t1 • • is acceleration of the bogie 12a in the right and left direction. c'
2 is a damping constant of a lateral movement damper. h
4 is a distance between the center of gravity of the bogie 12a and the lateral movement
damper in the up and down direction. y
b • is a velocity of the vehicle body 11 in the right and left direction. L represents
1/2 of the interval between the center of the bogie 12a and the center of the bogie
12b in the forward and backward direction (the interval between the center of the
bogie 12a and the center of the bogie 12b in the forward and backward direction becomes
2L).
φb • is an angular velocity of the vehicle body 11 in the yawing direction. h
5 is a distance between the lateral movement damper and the center of gravity of the
vehicle body 11 in the up and down direction.
φb • is an angular velocity of the vehicle body 11 in the rolling direction. y
w2 • is a velocity of the wheel set 13b in the right and left direction. k'
2 is a spring constant of the air spring (bolster spring) in the right and left direction.
h
2 is a distance between the center of gravity of each of the bogies 12a, 12b and the
center of the air spring (bolster spring) in the up and down direction. y
b is a displacement of the vehicle body 11 in the right and left direction.
φb is a pivot amount (angular displacement) of the vehicle body 11 in the yawing direction.
h
3 is a distance between the center of the air spring (bolster spring) and the center
of gravity of the vehicle body 11 in the up and down direction.
φb is a pivot amount (angular displacement) of the vehicle body 11 in the rolling direction.
Note that respective variables in (10) Equation are represented by being replaced
with the variables in (9) Equation according to the meanings of the subscripts described
above.
[Yawing of bogie]
[0039] The motion equations that describe the yawings of the bogies 12a, 12b are expressed
by (11) Equation and (12) Equation below.
[Mathematical equation 4]

[0040] I
Tz is a moment of inertia of the bogies 12a, 12b in the yawing direction.
φt1 • • is angular acceleration of the bogie 12a in the yawing direction.
φw2 • is an angular velocity of the wheel set 13b in the yawing direction.
φw2 is a pivot amount (angular displacement) of the wheel set 13b in the yawing direction.
y
w2 is a displacement of the wheel set 13b in the right and left direction. k'
0 is stiffness of a rubber bush of the yaw damper. b'
0 represents 1/2 of the interval between the two yaw dampers, which are disposed on
the right and left sides of each of the bogies 12a, 12b, in the right and left direction
(the interval between the two yaw dampers, which are disposed on the right and left
sides of each of the bogies 12a, 12b, in the right and left direction becomes 2b'
0).
φy1 is a pivot amount (angular displacement) of the yaw damper disposed on the bogie
12a in the yawing direction. k"
2 is a spring constant of the air spring (bolster spring) in the forward and backward
direction. b
2 represents 1/2 of the interval between the two air springs (bolster springs), which
are disposed on the right and left sides of each of the bogies 12a, 12b, in the right
and left direction (the interval between the two air springs (bolster springs), which
are disposed on the right and left sides of each of the bogies 12a, 12b, in the right
and left direction becomes 2b
2). Note that respective variables in (12) Equation are represented by being replaced
with the variables in (11) Equation according to the meanings of the subscripts described
above.
[Rolling of bogie]
[0041] The motion equations that describe the rollings of the bogies 12a, 12b are expressed
by (13) Equation and (14) Equation below.
[Mathematical equation 5]

[0042] I
Tx is a moment of inertia of the bogies 12a, 12b in the rolling direction. φ
t1 • • is angular acceleration of the bogie 12a in the rolling direction. c
1 is a damping constant of an axle damper in the up and down direction. b'
1 represents 1/2 of the interval between the two axle dampers, which are disposed on
the right and left sides of each of the bogies 12a, 12b, in the right and left direction
(the interval between the two axle dampers, which are disposed on the right and left
sides of each of the bogies 12a, 12b, in the right and left direction becomes 2b'
1). c
2 is a damping constant of the air spring (bolster spring) in the up and down direction.
φa1 • is an angular velocity of the air spring (bolster spring) disposed on the bogie
12a in the rolling direction. k
1 is a spring constant of an axle spring in the up and down direction.
λ is a value obtained by dividing the volume of the air spring (bolster spring) main
body by the volume of an auxiliary air chamber. k
2 is a spring constant of the air spring (bolster spring) in the up and down direction.
φa1 is a pivot amount (angular displacement) of the air spring (bolster spring) disposed
on the bogie 12a in the rolling direction. k
3 is equivalent stiffness by a change in effective pressure receiving area of the air
spring (bolster spring). Note that respective variables in (14) Equation are represented
by being replaced with the variables in (13) Equation according to the meanings of
the subscripts described above. Note that
φa2 is a pivot amount (angular displacement) of the air spring (bolster spring) disposed
on the bogie 12b in the rolling direction.
[Transversal vibration of vehicle body]
[0043] The motion equation that describes the transversal vibration of the vehicle body
11 (motion in the right and left direction) is expressed by (15) Equation below.
[Mathematical equation 6]

[0044] m
B is the mass of the bogies 12a, 12b. y
b • • is acceleration of the vehicle body 11 in the right and left direction. y
t2 • is a velocity of the bogie 12b in the right and left direction.
φt2 • is an angular velocity of the bogie 12b in the rolling direction. y
t2 is a displacement of the bogie 12b in the right and left direction.
φt2 is a pivot amount (angular displacement) of the bogie 12b in the rolling direction.
[Yawing of vehicle body]
[0045] The motion equation that describes the yawing of the vehicle body 11 is expressed
by (16) Equation below.
[Mathematical equation 7]

[0046] I
Bz is a moment of inertia of the vehicle body 11 in the yawing direction.
φb • • is angular acceleration of the vehicle body 11 in the yawing direction. c
0 is a damping constant of the yaw damper in the forward and backward direction.
φy1 • is an angular velocity of the yaw damper disposed on the bogie 12a in the yawing
direction.
φy2 • is an angular velocity of the yaw damper disposed on the bogie 12b in the yawing
direction.
φt2 is a pivot amount (angular displacement) of the bogie 12b in the yawing direction.
[Rolling of vehicle body]
[0047] The motion equation that describes the rolling of the vehicle body 11 is expressed
by (17) Equation below.
[Mathematical equation 8]

[0048] I
Bx is a moment of inertia of the vehicle body 11 in the rolling direction.
φb • • is angular acceleration of the vehicle body 11 in the rolling direction.
[Yawing of yaw damper]
[0049] The motion equations that describe the yawing of the yaw damper disposed on the bogie
12a and the yawing of the yaw damper disposed on the bogie 12b are expressed by (18)
Equation and (19) Equation below respectively.
[Mathematical equation 9]

[0050] φy2 is a pivot amount (angular displacement) of the yaw damper disposed on the bogie
12b in the yawing direction.
[Rolling of air spring (bolster spring)]
[0051] The motion equations that describe the rolling of the air spring (bolster spring)
disposed on the bogie 12a and the rolling of the air spring (bolster spring) disposed
on the bogie 12b are expressed by (20) Equation and (21) Equation below respectively.
[Mathematical equation 10]

[0052] φa2 • is an angular velocity of the air spring (bolster spring) disposed on the bogie
12b in the rolling direction.
(Forward-and-backward-direction force)
[0053] Next, the forward-and-backward-direction force will be explained. Note that the forward-and-backward-direction
force itself is the same as that described in Patent Literature 1.
[0054] In-phase components of the longitudinal creep force in one wheel of right and left
wheels in one wheel set and the longitudinal creep force in the other wheel are components
corresponding to a braking force and a driving force. Accordingly, the forward-and-backward-direction
force is preferably determined so as to correspond to an opposite-phase component
of the longitudinal creep force. The opposite-phase component of the longitudinal
creep force is a component to be opposite in phase to each other between the longitudinal
creep force in one wheel of the right and left wheels in one wheel set and the longitudinal
creep force in the other wheel. That is, the opposite-phase component of the longitudinal
creep force is a component, of the longitudinal creep force, in the direction in which
the axle is twisted. In this case, the forward-and-backward-direction force becomes
a component opposite in phase to each other out of forward-and-backward-direction
components of forces that occur in the aforementioned two members attached to both
the right and left sides of one wheel set.
[0055] Hereinafter, there will be explained concrete examples of the forward-and-backward-direction
force in the case where the forward-and-backward-direction force is determined so
as to correspond to the opposite-phase component of the longitudinal creep force.
[0056] In the case of the axle box suspension being a mono-link type axle box suspension,
the axle box suspension includes a link, and the axle box and the bogie frame are
coupled by the link. A rubber bush is attached to both ends of the link. In this case,
the forward-and-backward-direction force becomes, out of forward-and-backward-direction
components of loads that two links, which are attached to right and left ends of one
wheel set one by one, receive, the component to be opposite in phase to each other.
Further, due to arrangement and constitution of the links, the link mainly receives,
out of loads in the forward and backward direction, the right and left direction,
and the up and down direction, the load in the forward and backward direction. Accordingly,
one strain gauge only needs to be attached to each link, for example. By using a measured
value of the strain gauge, the forward-and-backward-direction component of the load
that this link receives is derived, to thereby obtain a measured value of the forward-and-backward-direction
force. Further, in place of applying such a design, a forward-and-backward-direction
displacement of the rubber bush attached to the link may be measured by a displacement
meter. In this case, the product of a measured displacement and a spring constant
of this rubber bush is set as the measured value of the forward-and-backward-direction
force. In the case of the axle box suspension being the mono-link type axle box suspension,
the previously-described member for supporting the axle box becomes the link or the
rubber bush.
[0057] Note that the load measured by the strain gauge attached to the link sometimes includes
not only the component in the forward and backward direction, but also at least one
component of a component in the right and left direction and a component in the up
and down direction. However, even in such a case, due to the structure of the axle
box suspension, the load of the component in the right and left direction and the
load of the component in the up and down direction that the link receives are sufficiently
smaller than the load of the component in the forward and backward direction. Accordingly,
only attaching one strain gauge to each link makes it possible to obtain a measured
value of the forward-and-backward-direction force, which has accuracy to be required
practically. In this manner, the components other than the component in the forward
and backward direction are sometimes included in the measured value of the forward-and-backward-direction
force. Therefore, three or more strain gauges may be attached to each link so as to
cancel the strains in the up and down direction and the right and left direction.
This makes it possible to improve the accuracy of the measured value of the forward-and-backward-direction
force.
[0058] In the case of the axle box suspension being an axle beam type axle box suspension,
the axle box suspension includes an axle beam, and the axle box and the bogie frame
are coupled by the axle beam. The axle beam may be formed integrally with the axle
box. A rubber bush is attached to a bogie frame-side end of the axle beam. In this
case, the forward-and-backward-direction force becomes, out of forward-and-backward-direction
components of loads that two axle beams, which are attached to right and left ends
of one wheel set one by one, receive, the component to be opposite in phase to each
other. Further, due to arrangement and constitution of the axle beams, the axle beam
is likely to receive, out of loads in the forward and backward direction, the right
and left direction, and the up and down direction, the load in the right and left
direction, in addition to the load in the forward and backward direction. Accordingly,
two or more strain gauges are attached to each axle beam so as to cancel the strain
in the right and left direction, for example. By using measured values of these strain
gauges, the forward-and-backward-direction component of the load that the axle beam
receives is derived, to thereby obtain a measured value of the forward-and-backward-direction
force. Further, in place of applying such a design, a forward-and-backward-direction
displacement of the rubber bush attached to the axle beam may be measured by a displacement
meter. In this case, the product of a measured displacement and a spring constant
of this rubber bush is set as the measured value of the forward-and-backward-direction
force. In the case of the axle box suspension being the axle beam type axle box suspension,
the previously-described member for supporting the axle box becomes the axle beam
or the rubber bush.
[0059] Note that the load measured by the strain gauge attached to the axle beam sometimes
includes not only the components in the forward and backward direction and the right
and left direction, but also the component in the up and down direction. However,
even in such a case, due to the structure of the axle box suspension, the load of
the component in the up and down direction that the axle beam receives is sufficiently
smaller than the load of the component in the forward and backward direction and the
load of the component in the right and left direction. Accordingly, even if the strain
gauge is not attached so as to cancel the load of the component in the up and down
direction that the axle beam receives, a measured value of the forward-and-backward-direction
force, which has accuracy to be required practically, can be obtained. In this manner,
the components other than the component in the forward and backward direction are
sometimes included in the measured forward-and-backward-direction force, and thus
three or more strain gauges may be attached to each axle beam so as to cancel the
strain in the up and down direction as well as the strain in the right and left direction.
This makes it possible to improve the accuracy of the measured value of the forward-and-backward-direction
force.
[0060] In the case of the axle box suspension being a leaf spring type axle box suspension,
the axle box suspension includes a leaf spring, and the axle box and the bogie frame
are coupled by the leaf spring. A rubber bush is attached to ends of the leaf spring.
In this case, the forward-and-backward-direction force becomes, out of forward-and-backward-direction
components of loads that two leaf springs, which are attached to right and left ends
of one wheel set one by one, receive, the component to be opposite in phase to each
other. Further, due to arrangement and constitution of the leaf springs, the leaf
spring is likely to receive, out of loads in the forward and backward direction, the
right and left direction, and the up and down direction, the load in the right and
left direction and the load in the up and down direction, in addition to the load
in the forward and backward direction. Accordingly, three or more strain gauges are
attached to each leaf spring so as to cancel the strains in the right and left direction
and the up and down direction, for example. By using measured values of these strain
gauges, the forward-and-backward-direction component of the load that the leaf spring
receives is derived, to thereby obtain a measured value of the forward-and-backward-direction
force. Further, in place of applying such a design, a forward-and-backward-direction
displacement of the rubber bush attached to the leaf spring may be measured by a displacement
meter. In this case, the product of a measured displacement and a spring constant
of this rubber bush is set as the measured value of the forward-and-backward-direction
force. In the case of the axle box suspension being the leaf spring type axle box
suspension, the previously-described member for supporting the axle box becomes the
leaf spring or the rubber bush.
[0061] Note that as the previously-described displacement meter, a well-known laser displacement
meter or eddy current displacement meter can be used.
[0062] Further, the forward-and-backward-direction force has been explained here by taking
the case of the system of the axle box suspension being a mono-link type, an axle
beam type, and a leaf spring type as an example. However, the system of the axle box
suspension is not limited to the mono-link type, the axle beam type, and the leaf
spring type. In conformity with the system of the axle box suspension, the forward-and-backward-direction
force can be determined in the same manner as in the mono-link type, the axle beam
type, and the leaf spring type.
[0063] Further, the case where a measured value of a single forward-and-backward-direction
force can be obtained in one wheel set will be explained as an example, in order to
simplify the explanation below. That is, the railway vehicle illustrated in Fig. 1
has the four wheel sets 13a to 13d. Accordingly, it is possible to obtain measured
values of four forward-and-backward-direction forces T
1 to T
4.
(First embodiment)
[0064] Next, a first embodiment of the present invention will be described.
<Inspection apparatus 500>
[0065] Fig. 5 is a view illustrating one example of a functional configuration of an inspection
apparatus 500. Fig. 6 is a view illustrating one example of a hardware configuration
of the inspection apparatus 500. Fig. 7 is a flowchart illustrating one example of
processing in the inspection apparatus 500. In the present embodiment, as illustrated
in Fig. 1, the case where the inspection apparatus 500 is mounted on the railway vehicle
will be explained as an example.
[0066] In Fig. 5, the inspection apparatus 500 includes, as its functions, a storage unit
501, a data acquisition unit 502, a first frequency adjustment unit 503, a state variable
derivation unit 504, a second frequency adjustment unit 505, a track state derivation
unit 506, and an output unit 507.
[0067] In Fig. 6, the inspection apparatus 500 includes a CPU 601, a main memory 602, an
auxiliary memory 603, a communication circuit 604, a signal processing circuit 605,
an image processing circuit 606, an I/F circuit 607, a user interface 608, a display
609, and a bus 610.
[0068] The CPU 601 overall controls the entire inspection apparatus 500. The CPU 601 uses
the main memory 602 as a work area to execute a program stored in the auxiliary memory
603. The main memory 602 stores data temporarily. The auxiliary memory 603 stores
various kinds of data, in addition to programs to be executed by the CPU 601. The
auxiliary memory 603 stores later-described state equations and observation equations.
The storage unit 501 is fabricated by using the CPU 601 and the auxiliary memory 603,
for example.
[0069] The communication circuit 604 is a circuit intended for performing communication
with the outside of the inspection apparatus 500. The communication circuit 604 receives
information of the measured value of the forward-and-backward-direction force, for
example. The communication circuit 604 may perform radio communication or wire communication
with the outside of the inspection apparatus 500.
The communication circuit 604 is connected to an antenna provided on the railway vehicle
in the case of performing radio communication.
[0070] The signal processing circuit 605 performs various kinds of signal processing on
signals received by the communication circuit 604 and signals input according to the
control made by the CPU 601. The data acquisition unit 502 is fabricated by using
the CPU 601, the communication circuit 604, and the signal processing circuit 605,
for example. Further, the first frequency adjustment unit 503, the state variable
derivation unit 504, the second frequency adjustment unit 505, and the track state
derivation unit 506 are fabricated by using the CPU 601 and the signal processing
circuit 605, for example.
[0071] The image processing circuit 606 performs various kinds of image processing on signals
input according to the control made by the CPU 601. The signal after being subjected
to the image processing is output to the display 609.
[0072] The user interface 608 is a part through which an operator gives an instruction to
the inspection apparatus 500. The user interface 608 includes buttons, switches, dials,
and so on, for example. Further, the user interface 608 may include a graphical user
interface using the display 609.
[0073] The display 609 displays an image based on a signal output from the image processing
circuit 606. The I/F circuit 607 exchanges data with a device connected to the I/F
circuit 607. In Fig. 6, as the device to be connected to the I/F circuit 607, the
user interface 608 and the display 609 are illustrated. However, the device to be
connected to the I/F circuit 607 is not limited to these. For example, a portable
storage medium may be connected to the I/F circuit 607. Further, at least a part of
the user interface 608 and the display 609 may be provided outside the inspection
apparatus 500.
[0074] The output unit 507 is fabricated by using at least any one of a set including the
communication circuit 604, and the signal processing circuit 605, and a set including
the image processing circuit 606, the I/F circuit 607, and the display 609, for example.
[0075] Note that the CPU 601, the main memory 602, the auxiliary memory 603, the signal
processing circuit 605, the image processing circuit 606, and the I/F circuit 607
are connected to the bus 610. Communication among these components is performed via
the bus 610. Further, the hardware of the inspection apparatus 500 is not limited
to the one illustrated in Fig. 6 as long as it can realize later-described functions
of the inspection apparatus 500.
[Storage unit 501]
[0076] The storage unit 501 stores equations which are used when the later-described state
variable derivation unit 504 derives the state variables.
[0077] In the present embodiment, the storage unit 501 stores state equations and observation
equations.
[0078] In the present embodiment, the case of using the state equations and the observation
equations described in Patent Literature 1 will be explained as an example.
[0079] First, the state equation will be described.
[0080] In the present embodiment, (5) Equation to (8) Equation (the motion equations that
describe the yawings of the wheel sets 13a to 13d) are not included in the state equation,
and the state equation is constituted as follows.
[0081] First, (9) Equation and (10) Equation (the motion equations that describe the transversal
vibrations of the bogies 12a, 12b (motion in the right and left direction)), (13)
Equation and (14) Equation (the motion equations that describe the rollings of the
bogies 12a, 12b), (15) Equation (the motion equation that describes the transversal
vibration of the vehicle body 11 (motion in the right and left direction)), (16) Equation
(the motion equation that describes the yawing of the vehicle body 11), (17) Equation
(the motion equation that describes the rolling of the vehicle body 11), (18) Equation
and (19) Equation (the motion equations that describe the yawings of the yaw damper
disposed on the bogie 12a and the yaw damper disposed on the bogie 12b), and (20)
Equation and (21) Equation (the motion equations that describe the rollings of the
air spring (bolster spring) disposed on the bogie 12a and the air spring (bolster
spring) disposed on the bogie 12b) are used as they are to constitute the state equation.
[0082] Meanwhile, in (1) Equation to (4) Equation (the motion equations that describe the
transversal vibrations of the wheel sets 13a to 13d (motion in the right and left
direction)) and (11) Equation and (12) Equation (the motion equations that describe
the yawings of the bogies 12a, 12b), the pivot amounts (angular displacements)
φw1 to
φw4 and the angular velocities
φw1 • to
φw4 • of the wheel sets 13a to 13d in the yawing direction are included. Results obtained
after eliminating these variables from (1) Equation to (4) Equation, (11) Equation,
and (12) Equation are used to constitute the state equation.
[0083] First, the forward-and-backward-direction forces T
1 to T
4 of the wheel sets 13a to 13d are expressed by (22) Equation to (25) Equation below.
[0084] In this manner, the forward-and-backward-direction forces T
1 to T
4 are determined according to the differences between the angular displacements
φw1 to
φw4 of the wheel sets in the yawing direction and the angular displacements
φt1 and
φt2 of the bogies on which these wheel sets are provided in the yawing direction.
[Mathematical equation 11]

[0085] Transformation variables e
1 to e
4 are defined as in (26) Equation to (29) Equation below. As above, the transformation
variables e
1 to e
4 are defined by the differences between the angular displacements
φt1 and
φt2 of the bogies in the yawing direction and the angular displacements
φw1 to
φw4 of the wheel sets in the yawing direction. The transformation variables e
1 to e
4 are variables for performing mutual transformation between the angular displacements
φt1 and
φt2 of the bogies in the yawing direction and the angular displacements
φw1 to
φw4 of the wheel sets in the yawing direction.
[Mathematical equation 12]

[0088] As above, (1) Equation to (4) Equation (the motion equations that describe the transversal
vibrations of the wheel sets 13a to 13d (motion in the right and left direction))
are expressed by using the transformation variables e
1 to e
4, thereby making it possible to eliminate the pivot amounts (angular displacements)
φw1 to
φw4 of the wheel sets 13a to 13d in the yawing direction that are included in these motion
equations.
[0089] When (22) Equation to (25) Equation are substituted into (11) Equation and (12) Equation
(the motion equations that describe the yawings of the bogies 12a, 12b), (38) Equation
and (39) Equation below are obtained.
[Mathematical equation 15]

[0090] As above, (11) Equation and (12) Equation (the motion equations that describe the
yawings of the bogies 12a, 12b) are expressed by using the forward-and-backward-direction
forces T
1 to T
4, thereby making it possible to eliminate the angular displacements
φw1 to
φw4 and the angular velocities
φ w1. to
φw4. of the wheel sets 13a to 13d in the yawing direction that are included in these
motion equations.
[0092] As above, in the present embodiment, as in (34) Equation to (37) Equation, the motion
equations that describe the transversal vibrations of the wheel sets 13a to 13d (motion
in the right and left direction) are expressed, and at the same time, as in (38) Equation
and (39) Equation, the motion equations that describe the yawings of the bogies 12a,
12b are expressed. The state equation is constituted by using (34) Equation to (39)
Equation. Further, (40) Equation to (43) Equation are ordinary differential equations.
Actual values of the transformation variables e
1 to e
4, which are solutions of the ordinary differential equations, can be derived by using
the values of the forward-and-backward-direction forces T
1 to T
4 in the wheel sets 13a to 13d. Here, the values of the forward-and-backward-direction
forces T
1 to T
4 are obtained by reducing a signal strength of a low-frequency component to be generated
due to the railway vehicle traveling on the curved portion of the track from the time-series
data of the measured value of the forward-and-backward-direction force, with the use
of the later-described first frequency adjustment unit 503.
[0093] The actual values of the transformation variables e
1 to e
4 derived as above are given to (34) Equation to (37) Equation. Further, the values
of the forward-and-backward-direction forces T
1 to T
4 in the wheel sets 13a to 13d are given to (38) Equation and (39) Equation. Here,
the values of the forward-and-backward-direction forces T
1 to T
4 are obtained by reducing a signal strength of a low-frequency component to be generated
due to the railway vehicle traveling on the curved portion of the track from the time-series
data of the measured value of the forward-and-backward-direction force, with the use
of the later-described first frequency adjustment unit 503.
[0094] In the present embodiment, variables illustrated in (44) Equation below are set as
the state variables, and by using the motion equations of (9) Equation, (10) Equation,
(13) Equation to (21) Equation, and (34) Equation to (39) Equation, the state equation
is constituted.
[Mathematical equation 17]

[0095] The storage unit 501 receives the state equation constituted as above, for example,
based on the operation of the user interface 608 made by an operator and stores it.
[0096] Next, the observation equation will be described.
[0097] In the present embodiment, the acceleration of the vehicle body 11 in the right and
left direction, the accelerations of the bogies 12a, 12b in the right and left direction,
and the accelerations of the wheel sets 13a to 13d in the right and left direction
are set to observation variables. These observation variables are observation variables
of filtering by a later-described Kalman filter. In the present embodiment, (34) Equation
to (37) Equation, (9) Equation, (10) Equation, and (15) Equation (the motion equations
that describe the transversal vibrations) are used to constitute an observation equation.
[0098] The storage unit 501 receives the observation equation constituted in this manner,
for example, based on the operation of the user interface 608 made by an operator
and stores it.
[0099] After the state equation and the observation equation are stored in the inspection
apparatus 500 as above, the data acquisition unit 502, the first frequency adjustment
unit 503, the state variable derivation unit 504, the second frequency adjustment
unit 505, the track state derivation unit 506, and the output unit 507 start. Specifically,
the processing according to the flowchart in Fig. 7 starts after the state equation
and the observation equation are stored in the inspection apparatus 500.
[Data acquisition unit 502, S701]
[0100] The data acquisition unit 502 acquires time-series data of the measured value of
the forward-and-backward-direction force. The method of measuring the forward-and-backward-direction
force is as described previously. The data acquisition unit 502 can acquire the time-series
data of the measured value of the forward-and-backward-direction force by performing
communication with an arithmetic device that calculates the forward-and-backward-direction
force by using a measured value of a strain gauge for measuring the forward-and-backward-direction
force, for example. Note that the data acquisition unit 502 does not acquire time-series
data of a measured value of the acceleration of the vehicle body 11 in the right and
left direction, time-series data of measured values of the accelerations of the bogies
12a, 12b in the right and left direction, and time-series data of measured values
of the accelerations of the wheel sets 13a to 13d in the right and left direction.
[First frequency adjustment unit 503, S702]
[0101] The first frequency adjustment unit 503 reduces (preferably removes) the signal strength
of the low-frequency component included in the time-series data of the measured value
of the forward-and-backward-direction force acquired by the data acquisition unit
502. A signal of this low-frequency component is a signal that is not measured when
the railway vehicle is traveling on the linear track whose curvature is 0 (zero),
but is measured when the railway vehicle is traveling on the curved track. That is,
the signal measured when the railway vehicle is traveling on the curved track can
be regarded as a signal obtained by superimposing the signal of this low-frequency
component on the signal measured when the railway vehicle is traveling on the linear
track whose curvature is 0 (zero).
[0102] The present inventors devised a model in which an AR (Auto-regressive) model is corrected.
Further, the present inventors came up with an idea of reducing the signal strength
of the low-frequency component included in the time-series data of the measured value
of the forward-and-backward-direction force by using this model. In the following
explanation, the model devised by the present inventors is referred to as a corrected
AR model. In contrast to this, the well-known AR model is referred to as an AR model
simply. Hereinafter, there will be explained one example of the corrected AR model.
[0103] A value of time-series data of a physical quantity y at a time k (1 ≦ k ≦ M) is set
to y
k. M is a number indicating, as the time-series data of the physical quantity y, data
until when is contained, and is preset. In the following explanation, the time-series
data of the physical quantity will be abbreviated to data y as necessary. The AR model
approximating the value y
k of the data y is as in (45) Equation below, for example. The AR model is, as illustrated
in (45) Equation, an equation expressing a predicted value y^
k of the physical quantity at the time k (m+1 ≦ k ≦ M) in the data y by using an actual
value y
k-l of the physical quantity at a time k-l (1 ≦ l ≦ m) prior to the time k in the data
y. Note that y^
k is expressed by adding ^ above y
k in (45) Equation.
[Mathematical equation 18]

[0104] In (45) Equation,
α is a coefficient of the AR model. m is a number of the value of the data y to be
used for approximating the value y
k of the data y at the time k in the AR model, and is a number among values y
k-1 to y
k-m of the data y at continuous times k-1 to k-m prior to the time k. m is an integer
of less than M. As m, for example, 1500 can be used.
[0105] Subsequently, there is derived a conditional expression for approximating the predicted
value y^
k of the physical quantity at the time k by the AR model to the value y
k by using a least square method. As the condition for approximating the predicted
value y^
k of the physical quantity at the time k by the AR model to the value y
k, it is possible to employ a condition that minimizes a square error between the predicted
value y^
k of the physical quantity at the time k by the AR model and the value y
k, for example. That is, the least square method is used in order to approximate the
predicted value y^
k of the physical quantity at the time k by the AR model to the value y
k. (46) Equation below is a conditional expression for minimizing the square error
between the predicted value y^
k of the physical quantity at the time k by the AR model and the value y
k.
[Mathematical equation 19]

[0106] The relation of (47) Equation below is established by (46) Equation.
[Mathematical equation 20]

[0107] Further, (47) Equation is modified (expressed in matrix notation form), and thereby
(48) Equation below is obtained.
[Mathematical equation 21]

[0108] R
jl in (48) Equation is called autocorrelation of the data y, and is a value defined
by (49) Equation below. |j-l| at this time is referred to as a time lag.
[Mathematical equation 22]

[0109] Based on (48) Equation, (50) Equation below is considered. (50) Equation is an equation
derived from a condition that minimizes the error between the predicted value y^
k of the physical quantity at the time k by the AR model and the value y
k of the physical quantity at the time k corresponding to the predicted value y^
k. (50) Equation is called a Yule-Walker equation. Further, (50) Equation is a linear
equation in which a vector composed of coefficients of the AR model is set to a variable
vector. A constant vector on the left side in (50) Equation is a vector whose component
is the autocorrelation of the data y with a time lag of 1 to m. In the following explanation,
the constant vector on the left side in (50) Equation is referred to as an autocorrelation
vector as necessary. Further, a coefficient matrix on the right side in (50) Equation
is a matrix whose component is the autocorrelation of the data y with a time lag of
0 to m-1. In the following explanation, the coefficient matrix on the right side in
(50) Equation is referred to as an autocorrelation matrix as necessary.
[Mathematical equation 23]

[0110] Further, the autocorrelation matrix on the right side in (50) Equation (a matrix
of m×m composed of R
jl) is described as an autocorrelation matrix R as in (51) Equation below.
[Mathematical equation 24]

[0111] In general, when deriving the coefficient of the AR model, a method of solving (50)
Equation regarding a coefficient
α is used. In (50) Equation, the coefficient
α is derived so as to make the predicted value y^
k of the physical quantity at the time k derived by the AR model come close to the
value y
k of the physical quantity at the time k as much as possible. Therefore, frequency
characteristics of the AR model include a large number of frequency components included
in the value y
k of the data y at each time.
[0112] Accordingly, the present inventors focused on the autocorrelation matrix R to be
multiplied by the coefficient
α of the AR model and earnestly examined it. As a result of this, the present inventors
found out that it is possible to reduce the influence of a high-frequency component
included in the data y by using a part of eigenvalues of the autocorrelation matrix
R. That is, the present inventors found out that it is possible to rewrite the autocorrelation
matrix R so that the low-frequency component is emphasized.
[0113] There will be explained a concrete example of the above below.
[0114] The autocorrelation matrix R is subjected to singular value decomposition. Elements
of the autocorrelation matrix R are symmetric. Therefore, when the autocorrelation
matrix R is subjected to singular value decomposition, as in (52) Equation below,
the result becomes the product of an orthogonal matrix U, a diagonal matrix Σ, and
a transposed matrix of the orthogonal matrix U.
[Mathematical equation 25]

[0115] The diagonal matrix ∑ in (52) Equation is a matrix whose diagonal component is the
eigenvalues of the autocorrelation matrix R as illustrated in (53) Equation below.
The diagonal component of the diagonal matrix Σ is set to σ
11, σ
22, · · ·, σmm. Further, the orthogonal matrix U is a matrix in which each column component
vector is an eigenvector of the autocorrelation matrix R. The column component vector
of the orthogonal matrix U is set to u
1, u
2, ···, u
m. There is a correspondence relation in which the eigenvalue of the autocorrelation
matrix R responsive to an eigenvector u
j is σ
jj. The eigenvalue of the autocorrelation matrix R is a variable reflecting the strength
of each frequency component included in a time waveform of the predicted value y^
k of the physical quantity at the time k by the AR model.
[Mathematical equation 26]

[0116] The values of σ
11, σ
22, ···, σ
mm being the diagonal components of the diagonal matrix Σ obtained by the result of
the singular value decomposition of the autocorrelation matrix R are set in descending
order in order to simplify the illustration of the mathematical equation. A matrix
R' is defined as in (54) Equation below by using, out of the eigenvalues of the autocorrelation
matrix R illustrated in (53) Equation, s pieces of the eigenvalues, which are chosen
from the largest. s is a number that is 1 or more and less than m. In the present
embodiment, s is preset. The matrix R' is a matrix resulting from approximating the
autocorrelation matrix R by using s pieces of the eigenvalues out of the eigenvalues
of the autocorrelation matrix R.
[Mathematical equation 27]

[0117] A matrix U
s in (54) Equation is a matrix of m ×s composed of s pieces of the column component
vectors, which are chosen from the left of the orthogonal matrix U of (52) Equation
(eigenvectors corresponding to the eigenvalues to be used). That is, the matrix U
s is a submatrix composed of the left elements of m×s cut out from the orthogonal matrix
U. Further, U
sT in (54) Equation is a transposed matrix of U
s. U
sT is a matrix of s×m composed of s pieces of row component vectors, which are chosen
from the top of the matrix U
T in (52) Equation. The matrix Σ
s in (54) Equation is a matrix of s×s composed of s pieces of columns, which are chosen
from the left, and s pieces of rows, which are chosen from the top, of the diagonal
matrix Σ in (52) Equation. That is, the matrix Σ
s is a submatrix composed of the top and left elements of s×s cut out from the diagonal
matrix Σ.
[0118] When the matrix Σ
s and the matrix U
s are expressed by the matrix elements, (55) Equation below is obtained.
[Mathematical equation 28]

[0119] By using the matrix R' in place of the autocorrelation matrix R, the relational expression
of (50) Equation is rewritten into (56) Equation below.
[Mathematical equation 29]

[0120] (56) Equation is modified, and thereby (57) Equation below is obtained as the equation
for deriving the coefficient
α. The model that calculates the predicted value y^
k of the physical quantity at the time k from (45) Equation while using the coefficient
α derived by (57) Equation is the "corrected AR model".
[Mathematical equation 30]

[0121] The case where the values of σ
11, σ
22, ···, σ
mm being the diagonal components of the diagonal matrix Σ are set in descending order
has been explained here as an example. However, it is not necessary to set the diagonal
components of the diagonal matrix Σ in descending order during a process of calculating
the coefficient
α. In that case, the matrix U
s is not the submatrix composed of the left elements of m×s cut out from the orthogonal
matrix U, but becomes a submatrix composed of the cut out column component vectors
corresponding to the eigenvalues to be used (the eigenvectors). Further, the matrix
Σ
s is not the submatrix composed of the top and left elements of s×s cut out from the
diagonal matrix Σ, but becomes a submatrix to be cut out so as to make the eigenvalues
used for determining the coefficient of the corrected AR model become the diagonal
components.
[0122] (57) Equation is an equation to be used for determining the coefficient of the corrected
AR model. The matrix U
s in (57) Equation is a matrix (a third matrix) in which the eigenvectors corresponding
to the eigenvalues used for determining the coefficient of the corrected AR model
are set to the column component vectors, which is the submatrix of the orthogonal
matrix U obtained by the singular value decomposition of the autocorrelation matrix
R. Further, the matrix Σ
s in (57) Equation is a matrix (a second matrix) in which the eigenvalues used for
determining the coefficient of the corrected AR model are set to the diagonal components,
which is the submatrix of the diagonal matrix obtained by the singular value decomposition
of the autocorrelation matrix R. The matrix U
sΣ
sU
sT in (57) Equation is a matrix (a first matrix) derived from the matrix Σ
s and the matrix U
s.
[0123] The right side of (57) Equation is calculated, and thereby the coefficient
α of the corrected AR model is derived. One example of the method of deriving the coefficient
α of the corrected AR model has been explained above. Here, as the method of deriving
the coefficient of the AR model to be the base of the corrected AR model, the method
of using the least square method for the predicted value y^
k of the physical quantity at the time k has been set in order to make the method understandable
intuitively. However, there has been known a method of defining the AR model by using
the concept of a stochastic process and deriving its coefficient generally. In that
case, the autocorrelation is expressed by autocorrelation of the stochastic process
(a population). This autocorrelation of the stochastic process is expressed as a function
of a time lag. Therefore, the autocorrelation of the data y in the present embodiment
may be replaced with a value calculated by another calculating formula as long as
it approximates the autocorrelation of the stochastic process. For example, R
22 to R
mm are autocorrelation with a time lag of 0 (zero), but they may be replaced with R
11.
[0124] The number s of the eigenvalues extracted from the autocorrelation matrix R illustrated
in (53) Equation can be determined from a distribution of the eigenvalues of the autocorrelation
matrix R, for example.
[0125] As the physical quantity in the explanation of the previously-described corrected
AR model, the forward-and-backward-direction force is applied here. The value of the
forward-and-backward-direction force varies according to the state and the like of
the railway vehicle.
[0126] Accordingly, the railway vehicle is first made to travel on the track 16 to obtain
the data y of the measured value of the forward-and-backward-direction force. The
autocorrelation matrix R is derived by using (49) Equation and (51) Equation for each
of the obtained data y. The autocorrelation matrix R is subjected to singular value
decomposition expressed by (52) Equation, to thereby derive the eigenvalues of the
autocorrelation matrix R. Fig. 8 is a view illustrating one example of the distribution
of the eigenvalues of the autocorrelation matrix R. In Fig. 8, eigenvalues σ
11 to σ
mm, which are obtained by the autocorrelation matrix R in each of the time-series data
of the measured value y of the forward-and-backward-direction force T
1 in the wheel set 13a being subjected to singular value decomposition, are aligned
in ascending order and are plotted. In Fig. 8, the horizontal axis is an index of
the eigenvalue and the vertical axis is the value of the eigenvalue.
[0127] In the example illustrated in Fig. 8, there is one eigenvalue having significantly
high value when compared to the other values. Further, there are two eigenvalues whose
values are not so high when compared to the aforementioned eigenvalue having significantly
high value, but are relatively large when compared to the other values and thus cannot
be regarded as 0 (zero). Based on this, it is possible to employ two or three, for
example, as the number s of eigenvalues to be extracted from the autocorrelation matrix
R illustrated in (53) Equation. Even if either of them is employed, there is generated
no significant difference in the result. Note that the number of eigenvalue having
a value which is significantly higher than the other values may change depending on
the configuration of the railway vehicle, the configuration of the track, and so on.
Therefore, the number s of eigenvalues to be extracted from the autocorrelation matrix
R is not limited to these values as long as it is one or more.
[0128] The first frequency adjustment unit 503 performs the following processing every time
the data acquisition unit 502 acquires the value y
k of the time-series data of the measured value y of the forward-and-backward-direction
force at the time k at a predetermined sampling period.
[0129] First, the first frequency adjustment unit 503 generates the autocorrelation matrix
R by using (49) Equation and (51) Equation based on the time-series data of the measured
value y of the forward-and-backward-direction force and preset numbers M, m.
[0130] Next, the first frequency adjustment unit 503 performs singular value decomposition
on the autocorrelation matrix R, to thereby derive the orthogonal matrix U and the
diagonal matrix Σ of (52) Equation, and derives the eigenvalues σ
11 to σ
mm of the autocorrelation matrix R from the diagonal matrix Σ.
[0131] Next, the first frequency adjustment unit 503 chooses s pieces of the eigenvalues
σ
11 to σ
ss from the largest from among the plural eigenvalues σ
11 to σ
mm of the autocorrelation matrix R as the eigenvalues of the autocorrelation matrix
R to be used for deriving the coefficient
α of the corrected AR model.
[0132] Next, the first frequency adjustment unit 503 determines the coefficient
α of the corrected AR model by using (57) Equation based on the time-series data of
the measured value y of the forward-and-backward-direction force, the eigenvalues
σ
11 to σ
ss, and the orthogonal matrix U obtained by the singular value decomposition of the
autocorrelation matrix R.
[0133] Subsequently, the first frequency adjustment unit 503 derives the predicted value
y^
k of the time-series data of the measured value y of the forward-and-backward-direction
force at the time k from (45) Equation based on the coefficient
α of the corrected AR model and the time-series data of the measured value y of the
forward-and-backward-direction force. Time-series data of the predicted value y^
k of the forward-and-backward-direction force results in the time-series data from
which the low-frequency component included in the time-series data of the measured
value y of the forward-and-backward-direction force has been extracted.
[0134] Fig. 9 is a view illustrating one example of time-series data of measured values
of forward-and-backward-direction forces (measured values) and time-series data of
predicted values of the forward-and-backward-direction forces (calculated values).
Note that in the present embodiment, the measured values of the four forward-and-backward-direction
forces T
1 to T
4 are obtained. That is, four pieces of the data y of the forward-and-backward-direction
force are obtained. In Fig. 9, the measured value and the calculated value of each
of the four pieces of data y are illustrated. The horizontal axis in Fig. 9 indicates
a measuring time and a calculating time of the forward-and-backward-direction forces
T
1 to T
4, each of which is an elapsed time (second) from a reference time when the reference
time is set to 0 (zero). The vertical axis indicates the forward-and-backward-direction
forces T
1 to T
4 (Nm).
[0135] In Fig. 9, the calculated value of the forward-and-backward-direction force T
1 in the wheel set 13a is biased at about 15 seconds to 35 seconds. Specifically, the
calculated value of the forward-and-backward-direction force T
1 in the wheel set 13a exhibits, at about 15 seconds to 35 seconds, a value larger
than that at another time. This period corresponds to the period when the wheel set
13a passes through the curved track. The calculated value of the forward-and-backward-direction
force T
2 in the wheel set 13b, the calculated value of the forward-and-backward-direction
force T
3 in the wheel set 13c, and the calculated value of the forward-and-backward-direction
force T
4 in the wheel set 13d are also biased during the period when the wheel sets 13b, 13c,
13d pass through the curved track, similarly to the calculated value of the forward-and-backward-direction
force T
1 in the wheel set 13a.
[0136] Accordingly, in Fig. 9, removal of the calculated values from the measured values
of the forward-and-backward-direction forces T
1 to T
4 in the wheel sets 13a to 13d makes it possible to remove the low-frequency components,
which are due to the wheel sets 13a to 13d passing through the curved track, from
the signals of the forward-and-backward-direction forces T
1 to T
4. That is, in Fig. 9, when the calculated values are removed from the measured values
of the forward-and-backward-direction forces T
1 to T
4 in the wheel sets 13a to 13d, as the forward-and-backward-direction forces T
1 to T
4 when the wheel sets 13a to 13d have passed through the curved track, the forward-and-backward-direction
forces equivalent to those when the wheel sets 13a to 13d have passed through the
linear track can be obtained.
[0137] Accordingly, the first frequency adjustment unit 503 subtracts the time-series data
of the predicted value y^
k of the forward-and-backward-direction force from the time-series data (the data y)
of the measured value y
k of the forward-and-backward-direction force. In the following explanation, the time-series
data resulting from the subtraction of the time-series data of the predicted value
y^
k of the forward-and-backward-direction force from the time-series data (the data y)
of the measured value y
k of the forward-and-backward-direction force is referred to as time-series data of
a high-frequency component of the forward-and-backward-direction force as necessary.
Further, a value of the time-series data of the high-frequency component of the forward-and-backward-direction
force at each sampling time is referred to as a value of the high-frequency component
of the forward-and-backward-direction force as necessary.
[0138] Fig. 10 is a view illustrating one example of the time-series data of the high-frequency
components of the forward-and-backward-direction forces. The vertical axis in Fig.
10 indicates the time-series data of the high-frequency components of the forward-and-backward-direction
forces T
1, T
2, T
3, T
4. That is, the high-frequency components of the forward-and-backward-direction forces
T
1, T
2, T
3, T
4 illustrated on the vertical axis in Fig. 10 are ones obtained by subtracting the
calculated values from the measured values of the forward-and-backward-direction forces
T
1, T
2, T
3, T
4 in the wheel sets 13a, 13b, 13c, 13d that are illustrated in Fig. 9 respectively.
Further, the horizontal axis in Fig. 10 indicates a measuring time and a calculating
time of the forward-and-backward-direction forces T
1 to T
4, each of which is an elapsed time (second) from a reference time when the reference
time is set to 0 (zero), similarly to the horizontal axis in Fig. 9.
[0139] The first frequency adjustment unit 503 derives the time-series data of the high-frequency
components of the forward-and-backward-direction forces T
1 to T
4 as above.
[State variable derivation unit 504, S703]
[0140] The state variable derivation unit 504 sets the observation equation as the observation
equation stored by the storage unit 501, sets the state equation as the state equation
stored by the storage unit 501, and determines estimated values of the state variables
illustrated in (44) Equation by using the Kalman filter. At this time, the state variable
derivation unit 504 uses time-series data of the high-frequency components of the
forward-and-backward-direction forces T
1 to T
4 generated by the first frequency adjustment unit 503. In the present embodiment,
out of the time-series data of the measured value of the acceleration of the vehicle
body 11 in the right and left direction, the time-series data of the measured values
of the accelerations of the bogies 12a, 12b in the right and left direction, and the
time-series data of the measured values of the accelerations of the wheel sets 13a
to 13d in the right and left direction, at least the time-series data during a period
in which the measured values of the forward-and-backward-direction forces T
1 to T
4 have been obtained is not used when determining the estimated values of the state
variables.
[0141] The Kalman filter is one of the methods of performing data assimilation. That is,
the Kalman filter is one example of the method to determine an estimated value of
an unobserved variable (state variable) so as to reduce (minimize) the difference
between, of an observable variable (observation variable), a measured value and an
estimated value. The state variable derivation unit 504 derives a Kalman gain at which
the difference between, of the observation variable, the measured value and the estimated
value becomes small (minimum) and derives the estimated value of the unobserved variable
(state variable) at that time. In the Kalman filter, the following observation equation
of (58) Equation and the following state equation of (59) Equation are used.

[0142] In (58) Equation, Y is a vector in which the measured value of the observation variable
is stored. H is an observation model. X is a vector in which the state variable is
stored. V is observation noise. In (59) Equation, X· indicates a time differentiation
of X. Φ is a linear model. W is system noise. Note that the Kalman filter itself can
be fabricated by a well-known technique, and thus its detailed explanation is omitted.
[0143] In the technique described in Patent Literature 1, as the values to be given as the
measured values of the observation variables, the measured values (the measured value
of the acceleration of the vehicle body 11 in the right and left direction, the measured
values of the accelerations of the bogies 12a, 12b in the right and left direction,
and the measured values of the accelerations of the wheel sets 13a to 13d in the right
and left direction) are used as they are. In contrast to this, in the present embodiment,
as explained in the term of [first conception], not the measured value but a preset
fixed value is given as the value to be normally given as the measured value of the
observation variable when performing the data assimilation. In the present embodiment,
an average value of the pieces of time-series data of the accelerations is assumed
to be 0 (zero), and all of fixed values to be given as the observation variables are
set to 0 (zero). Therefore, in the present embodiment, when performing the data assimilation,
the state variable derivation unit 504 derives the estimated value of the state variable
so as to minimize an error of the estimated value of the observation variable with
respect to the fixed value (0 (zero) in this case) or minimize an expected value of
the error.
[0144] The state variable derivation unit 504 determines the estimated values of the state
variables illustrated in (44) Equation at a predetermined sampling period, to thereby
generate time-series data of the estimated values of the state variables illustrated
in (44) Equation.
[Second frequency adjustment unit 505, S704]
[0145] When the signal strength of the low-frequency component included in the time-series
data of the measured value of the forward-and-backward-direction force is not removed
sufficiently by the first frequency adjustment unit 503, the signal of the low-frequency
component due to the railway vehicle traveling on the curved track may remain in the
time-series data of the estimated values of the state variables generated by the state
variable derivation unit 504. Accordingly, the second frequency adjustment unit 505
reduces (preferably removes) the signal strength of the low-frequency component included
in the time-series data of the estimated values of the state variables generated by
the state variable derivation unit 504. Note that in the case where it is possible
to determine the number s of the eigenvalues to be extracted from the autocorrelation
matrix R illustrated in (53) Equation so as to sufficiently remove the signal strength
of the low-frequency component included in the time-series data of the measured value
of the forward-and-backward-direction force by the first frequency adjustment unit
503, the processing of the second frequency adjustment unit 505 is no longer required.
[0146] In the present embodiment, the second frequency adjustment unit 505 uses the corrected
AR model to reduce the signal strength of the low-frequency component included in
the time-series data of the estimated values of the state variables similarly to the
first frequency adjustment unit 503.
[0147] The second frequency adjustment unit 505 performs the following processing for each
state variable at a predetermined sampling period.
[0148] As the physical quantity in the explanation of the previously-described corrected
AR model, the state variable is applied here. That is, the data y of the state variable
results in the time-series data of the estimated values of the state variables generated
by the state variable derivation unit 504. Each of the estimated values of the state
variables varies according to the state of the railway vehicle.
[0149] First, the second frequency adjustment unit 505 generates the autocorrelation matrix
R by using (49) Equation and (51) Equation based on the data y of the estimated values
of the state variables and the preset numbers M and m.
[0150] Next, the second frequency adjustment unit 505 performs singular value decomposition
on the autocorrelation matrix R, to thereby derive the orthogonal matrix U and the
diagonal matrix Σ of (52) Equation, and derives the eigenvalues σ
11 to σ
mm of the autocorrelation matrix R from the diagonal matrix Σ.
[0151] Next, the second frequency adjustment unit 505 chooses s pieces of the eigenvalues
σ
11 to σ
ss from the largest from among the plural eigenvalues σ
11 to σ
mm of the autocorrelation matrix R as the eigenvalues of the autocorrelation matrix
R to be used for deriving the coefficient
α of the corrected AR model. s is preset for each state variable. The data y of the
estimated value of each state variable can be obtained in a manner as explained so
far in a state of causing the railway vehicle to travel on the track 16, for example.
Subsequently, a distribution of the eigenvalues of the autocorrelation matrix R is
made by the second frequency adjustment unit 505 individually for each state variable.
From the distributions of the eigenvalues of the autocorrelation matrix R, the second
frequency adjustment unit 505 determines the number s of the eigenvalues to be extracted
from the autocorrelation matrix R illustrated in (53) Equation for each of the state
variables.
[0152] Next, the second frequency adjustment unit 505 determines the coefficient
α of the corrected AR model by using (57) Equation based on the data y of the estimated
value of the state variable, the eigenvalues σ
11 to σ
ss, and the orthogonal matrix U obtained by the singular value decomposition of the
autocorrelation matrix R.
[0153] Subsequently, the second frequency adjustment unit 505 derives the predicted value
y^
k of the data y of the estimated value of the state variable at the time k from (45)
Equation based on the coefficient
α of the corrected AR model and the data y of the estimated value of the state variable.
Time-series data of the predicted value y^
k of the state variable results in the time-series data from which the low-frequency
component included in the data y of the estimated value of the state variable has
been extracted.
[0154] Subsequently, the second frequency adjustment unit 505 subtracts the time-series
data of the predicted value y^
k of the state variable from the data y of the estimated value of the state variable.
In the following explanation, a value of time-series data resulting from the subtraction
of the time-series data of the predicted value y^
k of the state variable from the data y of the estimated value of the state variable
at each sampling time is referred to as a value of a high-frequency component of the
state variable as necessary.
[Track state derivation unit 506, S705]
[0156] In the present embodiment, as illustrated in (60) Equation to (63) Equation, relational
expressions representing the relations between the forward-and-backward-direction
forces T
1 to T
4 and the alignment irregularity amounts y
R1 to y
R4 at the positions of the wheel sets 13a to 13d are set.
[0157] The track state derivation unit 506 calculates estimated values of the pivot amounts
(angular displacements)
φw1 to
φw4 of the wheel sets 13a to 13d in the yawing direction by (30) Equation to (33) Equation.
Subsequently, the track state derivation unit 506 gives the estimated values of the
pivot amounts (angular displacements)
φw1 to
φw4 of the wheel sets 13a to 13d in the yawing direction, the values of the high-frequency
components of the state variables generated by the second frequency adjustment unit
505, and the values of the high-frequency components of the forward-and-backward-direction
forces T
1 to T
4 generated by the first frequency adjustment unit 503 to (60) Equation to (63) Equation,
to thereby calculate the alignment irregularity amounts y
R1 to y
R4 at the positions of the wheel sets 13a to 13d. The state variables to be used here
are the displacements y
t1 and y
t2 of the bogies 12a, 12b in the right and left direction, the velocities y
t1· and y
t2· of the bogies 12a, 12b in the right and left direction, the displacements y
w1 to y
w4 of the wheel sets 13a to 13d in the right and left direction, and the velocities
y
w1· to y
w4· of the wheel sets 13a to 13d in the right and left direction. The track state derivation
unit 506 performs such a calculation of the alignment irregularity amounts y
R1 to y
R4 as above at a predetermined sampling period, to thereby obtain the time-series data
of the alignment irregularity amounts y
R1 to y
R4.
[0158] Subsequently, the track state derivation unit 506 calculates a final alignment irregularity
amount y
R from the alignment irregularity amounts y
R1 to y
R4. For example, the track state derivation unit 506 matches phases of the time-series
data of the alignment irregularity amounts y
R2 to y
R4 to a phase of the time-series data of the alignment irregularity amount y
R1. That is, the track state derivation unit 506 calculates, from the distance between
the wheel set 13a and the wheel sets 13b to 13d in the forward and backward direction
and the velocity of the railway vehicle, a delay time between the time when the wheel
set 13a passes through a certain position and the time when the wheel sets 13b to
13d pass through the certain position. The track state derivation unit 506 displaces
the phases of the time-series data of the alignment irregularity amounts y
R2 to y
R4 by this delay time.
[0159] The track state derivation unit 506 calculates an arithmetic mean value of the sum
of the values of the alignment irregularity amounts y
R1 to y
R4 whose phases are matched at the same sampling time as the final alignment irregularity
amount y
R at this sampling time. The track state derivation unit 506 performs such a calculation
at each sampling time, to thereby obtain time-series data of the final alignment irregularity
amount y
R. The phases of the alignment irregularity amounts y
R2 to y
R4 are matched to the phase of the alignment irregularity amount y
R1, thereby making it possible to cancel disturbance factors existing in common in the
time-series data of the alignment irregularity amounts y
R1 to y
R4.
[0160] Note that the track state derivation unit 506 may find a moving average of each of
the alignment irregularity amounts y
R1 to y
R4 whose phases are matched (namely, pass each of the alignment irregularity amounts
y
R1 to y
R4 through a low-pass filter) and calculate the final alignment irregularity amount
y
R from the alignment irregularity amounts y
R1 to y
R4 whose moving averages have been found.
[0161] Further, the track state derivation unit 506 may calculate, as the final alignment
irregularity amount y
R, an arithmetic mean value of two of the values of the alignment irregularity amounts
y
R1 to y
R4 whose phases are matched at the same sampling time from which the maximum value and
the minimum value are removed.
[0162] The inspection apparatus 500 uses the time-series data of the measured value of the
forward-and-backward-direction force at each sampling time acquired by the data acquisition
unit 502 while the railway vehicle is traveling in the traveling section being the
target of deriving the alignment irregularity amount, to execute pieces of the processing
of the first frequency adjustment unit 503, the state variable derivation unit 504,
the second frequency adjustment unit 505, and the track state derivation unit 506.
[0163] In this manner, the track state derivation unit 506 can obtain the alignment irregularity
amount y
R at each sampling time while the railway vehicle is traveling in the traveling section
being the target of deriving the alignment irregularity amount. The track state derivation
unit 506 calculates a traveling position of the railway vehicle at each sampling time
based on, for example, a traveling velocity of the railway vehicle and an elapsed
time from the time when the railway vehicle starts to travel. The traveling position
of the railway vehicle can be set to the position of the wheel set 13a, for example.
The track state derivation unit 506 derives the final alignment irregularity amount
y
R at each traveling position of the railway vehicle based on the alignment irregularity
amount y
R at each sampling time and the traveling position of the railway vehicle at each sampling
time.
[0164] Note that the track state derivation unit 506 does not always need to calculate the
traveling position of the railway vehicle at each sampling time as described previously.
For example, the track state derivation unit 506 may derive the traveling position
of the railway vehicle at each sampling time by using a GPS (Global Positioning System).
[Output unit 507, S706]
[0165] The output unit 507 outputs information of the final alignment irregularity amount
y
R that is calculated by the track state derivation unit 506. At this time, the output
unit 507 may output information indicating that the track 16 is abnormal in the case
where the final alignment irregularity amount y
R is larger than a preset value. As a form of output, it is possible to employ at least
any one of displaying the information on a computer display, transmitting the information
to an external device, and storing the information in an internal or external storage
medium, for example.
<Summary>
[0166] As described above, in the present embodiment, the inspection apparatus 500 gives
the measured values of the forward-and-backward-direction forces T
1 to T
4 and the actual values of the transformation variables e
1 to e
4 to the Kalman filter, to derive the state variables (y
w1· to y
w4·, y
w1 to y
w4, y
t1· and y
t2·, y
t1 and y
t2,
φt1· and
φt2·,
φt1 and
φt2,
φt1· and
φt2· ,
φt1 and
φt2, y
b·, y
b,
φb·,
φb,
φb·,
φb,
φy1,
φy2,
φa1,
φa2). At this time, the preset fixed value (0 (zero), for example) is used as the values
to be normally given as the measured values of the observation variables (the accelerations
of the vehicle body 11, the bogies 12a, 12b, and the wheel sets 13a to 13d in the
right and left direction) when performing the data assimilation. Next, the inspection
apparatus 500 uses the pivot amounts (angular displacements)
φt1 and
φt2 of the bogies 12a, 12b in the yawing direction included in the state variables and
the actual values of the transformation variables e
1 to e
4, to derive the pivot amounts (angular displacements)
φw1 to
φw4 of the wheel sets 13a to 13d in the yawing direction. Next, the inspection apparatus
500 substitutes the pivot amounts (angular displacements)
φw1 to
φw4 of the wheel sets 13a to 13d in the yawing direction, the state variables, and the
measured values of the forward-and-backward-direction forces T
1 to T
4 into the motion equations that describe the yawings of the wheel sets 13a to 13d,
to derive the alignment irregularity amounts y
R1 to y
R4 at the positions of the wheel sets 13a to 13d. Subsequently, the inspection apparatus
500 derives the final alignment irregularity amount y
R from the alignment irregularity amounts y
R1 to y
R4. Therefore, it is possible to derive the alignment irregularity amounts y
R1 to y
R4 (the final alignment irregularity amount y
R) without greatly decreasing accuracy, with no use of the measured values of the accelerations
of the vehicle body 11, the bogies 12a, 12b, and the wheel sets 13a to 13d in the
right and left direction. Therefore, it is possible to reduce the number of sensors
which are used for deriving the alignment irregularity amounts y
R1 to y
R4 (the final alignment irregularity amount y
R).
[0167] Further, in the present embodiment, the inspection apparatus 500 generates the autocorrelation
matrix R from the time-series data of the measured value y of the forward-and-backward-direction
force, and determines, by using s pieces of the eigenvalues from the largest chosen
from the eigenvalues obtained by the singular value decomposition of the autocorrelation
matrix R, the coefficient
α of the corrected AR model approximating the time-series data of the measured value
y of the forward-and-backward-direction force. Therefore, it is possible to determine
the coefficient
α so as to make the signal of the low-frequency component included in the time-series
data of the measured value y of the forward-and-backward-direction force remain and
prevent the high-frequency component from remaining. The inspection apparatus 500
calculates the predicted value y^
k of the forward-and-backward-direction force at the time k by giving the time-series
data of the measured value y of the forward-and-backward-direction force at the time
k-l (1 ≦ 1 ≦ m), which is prior to the time k, to the corrected AR model whose coefficient
α is determined in this manner. Therefore, it is possible to reduce the signal of the
low-frequency component, which is due to the railway vehicle traveling on the curved
track, from the time-series data of the measured value y of the forward-and-backward-direction
force without estimating a cutoff frequency beforehand. Subsequently, the inspection
apparatus 500 reduces the signal strength of the low-frequency components included
in the time-series data of the measured values of the forward-and-backward-direction
forces T
1 to T
4 in this manner and generates the time-series data of the high-frequency components
of the forward-and-backward-direction forces T
1 to T
4. The inspection apparatus 500 gives the time-series data of the high-frequency components
of the forward-and-backward-direction forces T
1 to T
4 to the relational expression between the forward-and-backward-direction forces T
1 to T
4 and the alignment irregularity amounts y
R1 to y
R4 at the positions of the wheel sets 13a to 13d, to thereby calculate the alignment
irregularity amounts y
R1 to y
R4 at the positions of the wheel sets 13a to 13d. This relational expression is an expression
based on the motion equations that describe the motions of the railway vehicle when
traveling on the linear track (namely, the equations not including the curvature radius
R of the track 16 (the rail)). Therefore, it is possible to detect the alignment irregularity
amounts y
R1 to y
R4 (the final alignment irregularity amount y
R) in the curved track based on the motion equations that describe the motions of the
railway vehicle when traveling on the linear track without using a special measuring
apparatus.
[Modified example]
[0168] In the present embodiment, the preset fixed value is given as the value to be normally
given as the measured value of the observation variable when performing the data assimilation.
This fixed value is not limited to 0 (zero). For example, it is also possible that
the time-series data of the measured value of the acceleration of the vehicle body
11 in the right and left direction, the time-series data of the measured values of
the accelerations of the bogies 12a, 12b in the right and left direction, and the
time-series data of the measured values of the accelerations of the wheel sets 13a
to 13d in the right and left direction when the railway vehicle having the inspection
apparatus 500 mounted thereon or a railway vehicle equivalent to this railway vehicle
(a railway vehicle whose structure is the same as that of this railway vehicle) travels
on the track 16 being the target of deriving the alignment irregularity amounts y
R1 to y
R4 (the final alignment irregularity amount y
R) are obtained, and an average value of the respective pieces of time-series data
is used as the fixed value. Further, by using these measured values, time-series data
of a predicted value of acceleration y^
k of the vehicle body 11 in the right and left direction, time-series data of predicted
values of accelerations y^
k of the bogies 12a, 12b in the right and left direction, and time-series data of predicted
values y^
k of accelerations of the wheel sets 13a to 13d in the right and left direction are
derived by the above-described corrected AR model. Subsequently, an average value
thereof may also be used as the fixed value. When it is designed as above, the measurement
of accelerations is performed, but this measurement is only required to be performed
once for each of the railway vehicle and the track 16, and measured values of accelerations
during a period in which the measured values of the forward-and-backward-direction
forces T
1 to T
4 in the wheel sets 13a to 13d have been obtained are not used when deriving the state
variables.
[0169] In the present embodiment, the case of using the corrected AR model has been explained
as an example. However, it is not always necessary to use the corrected AR model and
reduce the signal of the low-frequency component, which is due to the railway vehicle
traveling on the curved track, from the time-series data of the measured value y of
the forward-and-backward-direction force. For example, in the case where it is possible
to specify a frequency band due to the railway vehicle traveling on the curved track,
a high-pass filter may be used to reduce the signal of the low-frequency component,
which is due to the railway vehicle traveling on the curved track, from the time-series
data of the measured value y of the forward-and-backward-direction force. Further,
when the track on which the railway vehicle travels is a linear track (being an ideal
track whose curvature is 0 (zero)) or a track which is designed as a linear track
but has a curvature which is small enough to exert no influence on estimation accuracy
of the alignment irregularity amount, the processing of the first frequency adjustment
unit 503 and the processing of the second frequency adjustment unit 505 are no longer
required.
[0170] Further, in the present embodiment, the case where the wheel set to be a standard
when performing the phase matching is the wheel set 13a has been explained as an example.
However, the wheel set to be a standard may be the wheel set 13b, 13c, or 13d other
than the wheel set 13a.
[0171] Further, in the present embodiment, the case of using the Kalman filter has been
explained as an example. However, it is not always necessary to use the Kalman filter
as long as a filter that derives the estimated values of the state variables so that
the error of the estimated value of the observation variable with respect to the fixed
value becomes minimum or the expected value of this error becomes minimum (that is,
a filter that performs data assimilation) is used. For example, a particle filter
may be used. Note that as the error of the estimated value of the observation variable
with respect to the fixed value, for example, a square error between the estimated
value of the observation variable and the fixed value is cited.
[0172] Further, in the present embodiment, the case of deriving the alignment irregularity
amount has been explained as an example. However, it is not always necessary to derive
the alignment irregularity amount as long as information that reflects the track irregularity
(appearance failure of the track 16) is derived as information reflecting the state
of the track 16. For example, in addition to or in place of the alignment irregularity
amount, the following calculations of (64) Equation to (67) Equation may be performed,
to thereby derive a lateral force that occurs when the railway vehicle travels on
the linear track (stress in the right and left direction between the wheel and the
rail). Note that Q
1, Q
2, Q
3, Q
4 are lateral forces in the wheels 14a, 14b, 14c, 14d respectively. f
3 represents a spin creep coefficient.
[Mathematical equation 32]

[0173] Further, in the present embodiment, the case of including the state variables that
represent the state of the vehicle body 11 has been explained as an example. However,
the vehicle body 11 is a part into which vibrations by acting forces between the wheels
14a to 14d and the track 16 (creep force) propagate finally. Accordingly, it is not
necessary to include the state variables representing the state of the vehicle body
11 in the case where the influence by the propagation in the vehicle body 11 is judged
to be small, for example. In such a case, out of the motion equations of (1) Equation
to (21) Equation, (15) Equation to (17) Equation (the motion equations that describe
the transversal vibration, the yawing, and the rolling of the vehicle body 11) and
(18) Equation and (19) Equation (the motion equations that describe the yawing of
the yaw damper disposed on the bogie 12a and the yawing of the yaw damper disposed
on the bogie 12b) are no longer required. Further, in the motion equations of (1)
Equation to (21) Equation, the state amount relating to the vehicle body (state amount
including the subscript of b) and the value inside {} that includes the state amount
relating to the vehicle body (state amount including the subscript of b) (for example,
the third term {
φa2 -
φb} on the left side of (21) Equation)) are set to 0 (zero) .
[0174] Further, in the present embodiment, the case of the bogies 12a, 12b each being a
bolsterless bogie has been explained as an example. However, the bogies 12a, 12b are
not limited to the bolsterless bogies. Besides, according to the components of the
railway vehicle, forces that the railway vehicle receives, the directions of the motions
of the railway vehicle, or the like, the motion equations are rewritten appropriately.
That is, the motion equations are not limited to the ones exemplified in the present
embodiment. When the motion equation is set to represent that the railway vehicle
receives external force which does not depend on the state variables, the state equation
includes a term that represents this external force.
(Second embodiment)
[0175] Next, a second embodiment will be described. In the first embodiment, the case where
the state variables are derived by using the filter (Kalman filter) that performs
the data assimilation by setting the values to be normally given as the measured values
of the observation variables (the acceleration of the vehicle body 11 in the right
and left direction, the accelerations of the bogies 12a, 12b in the right and left
direction, and the accelerations of the wheel sets 13a to 13d in the right and left
direction) to the fixed value (0 (zero)), when performing the data assimilation, has
been described as an example. In contrast to this, in the present embodiment, a case
of deriving the state variables without performing the data assimilation will be described.
In this manner, the present embodiment and the first embodiment are different mainly
in the method of deriving the state variables (the function of the state variable
derivation unit 504). Therefore, in the explanation of the present embodiment, the
same reference numerals and symbols as those added to Fig. 1 to Fig. 10 are added
to the same parts as those in the first embodiment, or the like, and their detailed
explanations are omitted.
[0176] In the present embodiment, the storage unit 501 does not store the state equation
((58) Equation) and the observation equation ((59) Equation), but stores the following
motion equation of (68) Equation.

[0177] (68) Equation is one example of equation obtained by changing an equation representing
the motion equations of (9) Equation, (10) Equation, (13) Equation to (21) Equation,
and (34) Equation to (39) Equation by using the state variables illustrated in (44)
Equation (an equation corresponding to (68) Equation in which c is set to 1), so that
a temporal change in the state variables becomes smaller than that of this equation.
Concretely, (68) Equation is one obtained in a manner that, in an equation representing
the motion equations of (9) Equation, (10) Equation, (13) Equation to (21) Equation,
and (34) Equation to (39) Equation by using the state variables illustrated in (44)
Equation, a term which is connected to a term of first-order time differential (X·)
of the state variable by an equal sign is multiplied by a forgetting factor c. Specifically,
(68) Equation corresponds to the state equation of (59) Equation in which the forgetting
factor c is introduced, to thereby set the system noise W to 0 (zero).
[0178] The forgetting factor c is a preset value, and is (theoretically) a value of greater
than 0 and 1 or less (0 < c ≦ 1). The forgetting factor c functions in a manner that
the smaller the value thereof, the greater the degree of forgetfulness of a past observation
value. In (68) Equation, the smaller the value of the forgetting factor c, the smaller
the influence of the measured value of the forward-and-backward-direction force on
the estimated value (solution) of the state variable. For this reason, from a viewpoint
of correctly obtaining the estimated value (solution) of the state variable, the value
of the forgetting factor c is desirably close to 1. On the other hand, when the value
of the forgetting factor c is excessively large, there is a high possibility of divergence
of the estimated value (solution) of the state variable. In the present embodiment,
(68) Equation is directly solved without using the filter that performs the data assimilation.
Accordingly, there is a need to suppress the divergence of the estimated value (solution)
of the state variable. The value of the forgetting factor c is determined based on
the viewpoint as described above. As the forgetting factor c, for example, a value
of greater than 0.0 and 1.0 or less (0.0 < c ≦ 1.0), preferably a value of 0.90 or
more and 1.0 or less (0.90 ≦ c ≦ 1.0), more preferably a value of 0.95 or more and
1.0 or less (0.95 ≦ c ≦ 1.0), still more preferably a value of 0.99 or more and 1.0
or less (0.99 ≦ c ≦ 1.0), and most preferably 1.0 is selected among them.
[0179] However, it is essential that the forgetting factor c is selected so as to prevent
the divergence of the estimated value (solution) of the state variable obtained by
solving (68) Equation. If the divergence of the estimated value (solution) of the
state variable obtained by solving (68) Equation does not occur, the estimated value
(solution) of this state variable when the value of the forgetting factor is 1.0 becomes
the most accurate solution. However, when the value of the forgetting factor c is
1.0, it is highly likely that the estimated value (solution) of the state variable
obtained by solving (68) Equation diverges (the solution is not determined).
[0180] From such a viewpoint, the forgetting factor c may be selected by setting an upper
limit value of the forgetting factor c to less than 1.0. Specifically, the value of
the forgetting factor c can be selected from, for example, a value of greater than
0.0 and less than 1.0 (0.0 < c < 1.0), preferably a value of 0.90 or more and less
than 1.0 (0.90 ≦ c < 1.0), more preferably a value of 0.95 or more and less than 1.0
(0.95 ≦ c < 1.0), and still more preferably a value of 0.99 or more and less than
1.0 (0.99 ≦ c < 1.0).
[0181] Note that when the value of the forgetting factor c is 1.0, (68) Equation corresponds
to the motion equations themselves of (9) Equation, (10) Equation, (13) Equation to
(21) Equation, and (34) Equation to (39) Equation (an equation only representing the
motion equations by using the state variables).
[0182] The state variable derivation unit 504 uses the time-series data of the high-frequency
components of the forward-and-backward-direction forces T
1 to T
4 generated by the first frequency adjustment unit 503 to derive the actual values
of the transformation variables e
1 to e
4 and substitutes the actual values into (34) Equation to (37) Equation, and substitutes
the time-series data of the high-frequency components of the forward-and-backward-direction
forces T
1 to T
4 generated by the first frequency adjustment unit 503 into (38) Equation and (39)
Equation as the measured values of the forward-and-backward-direction forces T
1 to T
4 to solve the equation of (68) Equation, thereby determining the estimated values
of the state variables illustrated in (44) Equation. The method of solving the equation
of (68) Equation can be realized by a well-known numerical solution (Euler method
or the like), for example. Therefore, when deriving the estimated values of the state
variables, the state variable derivation unit 504 does not use the time-series data
of the measured value of the acceleration of the vehicle body 11 in the right and
left direction, the time-series data of the measured values of the accelerations of
the bogies 12a, 12b in the right and left direction, and the time-series data of the
measured values of the accelerations of the wheel sets 13a to 13d in the right and
left direction. Besides, the observation equation is also not used.
[0183] As described above, in the present embodiment, the inspection apparatus 500 gives
the measured values of the forward-and-backward-direction forces T
1 to T
4 and the actual values of the transformation variables e
1 to e
4 to the equation being the state equation with the system noise W set to 0 (zero)
in which the term other than the time differential term X· of the state variable is
multiplied by the forgetting factor c, to thereby derive the state variables (y
w1· to y
w4·, y
w1 to y
w4, y
t1· and y
t2·, y
t1 and y
t2,
φt1· and
φt2·,
φt1 and
φt2,
φt1· and
φt2·,
φt1 and
φt2, y
b·, y
b,
φb·,
φb,
φb·,
φb, φy1,
φy2,
φa1,
φa2). Therefore, it is possible to derive the alignment irregularity amounts y
R1 to y
R4 (the final alignment irregularity amount y
R) without greatly decreasing accuracy, with no use of the measured values of the accelerations
of the vehicle body 11, the bogies 12a, 12b, and the wheel sets 13a to 13d in the
right and left direction.
[0184] Also in the present embodiment, it is possible to employ the various modified examples
explained in the first embodiment. When the motion equation includes the external
force or the like that does not depend on the state equation X, (68) Equation is represented
as in the following (69) Equation.

[0185] G is a vector in which the term that does not depend on the state equation is stored.
f is a matrix corresponding to the vector G.
(Third embodiment)
[0186] Next, there will be explained a third embodiment.
[0187] In the first and second embodiments, the case where the inspection apparatus 500
mounted on the railway vehicle calculates the final alignment irregularity amount
y
R has been explained as an example. In contrast to this, in the present embodiment,
a data processing device in which some functions of the inspection apparatus 500 are
mounted is disposed in an operation center. The data processing device receives measured
data transmitted from the railway vehicle and calculates the final alignment irregularity
amount y
R by using the received measured data. In this manner, in the present embodiment, the
functions possessed by the inspection apparatus 500 in the first and second embodiments
are shared and executed by the railway vehicle and the operation center. Constitutions
and processing due to this are mainly different between the present embodiment and
the first and second embodiments. Accordingly, in the explanation of the present embodiment,
the same reference numerals and symbols as those added to Fig. 1 to Fig. 10 are added
to the same parts as those in the first and second embodiments, or the like, and their
detailed explanations are omitted. Note that the present embodiment can be applied
to any of the first and second embodiments.
[0188] Fig. 11 is a view illustrating one example of a configuration of an inspection system.
In Fig. 11, the inspection system includes data collecting devices 1110a, 1110b, and
a data processing device 1120. In Fig. 11, one example of functional configurations
of the data collecting devices 1110a, 1110b and the data processing device 1120 is
also illustrated. Note that each hardware of the data collecting devices 1110a, 1110b
and the data processing device 1120 can be fabricated by the one illustrated in Fig.
6, for example. Accordingly, detailed explanations of the hardware configurations
of the data collecting devices 1110a, 1110b and the data processing device 1120 are
omitted.
[0189] The data collecting devices 1110a, 1110b are mounted on each railway vehicle one
by one. The data processing device 1120 is disposed at the operation center. The operation
center centrally manages operations of a plurality of railway vehicles, for example.
<Data collecting devices 1110a, 1110b>
[0190] The data collecting devices 1110a, 1110b can be fabricated by the same components.
The data collecting devices 1110a, 1110b include data acquisition units 1111a, 1111b
and data transmission units 1112a, 1112b.
[Data acquisition units 1111a, 1111b]
[0191] The data acquisition units 1111a, 1111b have the same function as that of the data
acquisition unit 502. That is, the data acquisition units 1111a, 1111b acquire the
time-series data of the measured values of the forward-and-backward-direction forces,
similarly to the data acquisition unit 502. The configuration for obtaining the measured
value of the forward-and-backward-direction force is the same as that explained in
the first embodiment.
[Data transmission units 1112a, 1112b]
[0192] The data transmission units 1112a, 1112b transmit the time-series data of the measured
values of the forward-and-backward-direction forces acquired by the data acquisition
units 1111a, 1111b to the data processing device 1120. In the present embodiment,
the data transmission units 1112a, 1112b transmit the time-series data of the measured
values of the forward-and-backward-direction forces acquired by the data acquisition
units 1111a, 1111b to the data processing device 1120 by radio. At this time, the
data transmission units 1112a, 1112b add identification numbers of the railway vehicles
on which the data collecting devices 1110a, 1110b are mounted to the time-series data
of the measured values of the forward-and-backward-direction forces acquired by the
data acquisition units 1111a, 1111b. In this manner, the data transmission units 1112a,
1112b transmit the time-series data of the measured values of the forward-and-backward-direction
forces with the identification numbers of the railway vehicles added thereto.
<Data processing device 1120>
[Data reception unit 1121]
[0193] A data reception unit 1121 receives the time-series data of the measured values of
the forward-and-backward-direction forces transmitted by the data transmission units
1112a, 1112b. To the time-series data of the measured values of the forward-and-backward-direction
forces, the identification numbers of the railway vehicles, which are transmission
sources of the time-series data of the measured values of the forward-and-backward-direction
forces, have been added.
[Data storage unit 1122]
[0194] A data storage unit 1122 stores the time-series data of the measured values of the
forward-and-backward-direction forces received by the data reception unit 1121. The
data storage unit 1122 stores the time-series data of the measured value of the forward-and-backward-direction
force for each identification number of the railway vehicle. The data storage unit
1122 specifies the position of the railway vehicle at the time of receipt of the time-series
data of the measured value of the forward-and-backward-direction force based on the
current operation situation of the railway vehicle and the time of receipt of the
time-series data of the measured value of the forward-and-backward-direction force,
and stores information of the specified position and the time-series data of the measured
value of the forward-and-backward-direction force in association with each other.
Note that the data collecting devices 1110a, 1110b may collect the information of
the current positions of the railway vehicles and include the collected information
in the time-series data of the measured values of the forward-and-backward-direction
forces.
[Data reading unit 1123]
[0195] A data reading unit 1123 reads the time-series data of the measured value of the
forward-and-backward-direction force stored in the data storage unit 1122. The data
reading unit 1123 can read, out of the time-series data of the measured values of
the forward-and-backward-direction forces stored in the data storage unit 1122, data
designated by an operator. Further, the data reading unit 1123 can also read the time-series
data of the measured value of the forward-and-backward-direction force matching a
preset condition at a preset timing. In the present embodiment, the time-series data
of the measured value of the forward-and-backward-direction force read by the data
reading unit 1123 is determined based on at least any one of the identification number
and the position of the railway vehicle, for example.
[0196] A storage unit 501, a first frequency adjustment unit 503, a state variable derivation
unit 504, a second frequency adjustment unit 505, a track state derivation unit 506,
and an output unit 507 are the same as those explained in the first embodiment. Accordingly,
their detailed explanations are omitted here. Note that the first frequency adjustment
unit 503 uses the time-series data of the measured value of the forward-and-backward-direction
force read by the data reading unit 1123 in place of using the time-series data of
the measured value of the forward-and-backward-direction force acquired by the data
acquisition unit 502, and generates the time-series data of the high-frequency components
of the forward-and-backward-direction forces T
1 to T
4.
<Summary>
[0197] As described above, in the present embodiment, the data collecting devices 1110a,
1110b mounted on the railway vehicles collect the time-series data of the measured
values of the forward-and-backward-direction forces to transmit the data to the data
processing device 1120. The data processing device 1120 disposed at the operation
center stores the time-series data of the measured values of the forward-and-backward-direction
forces received from the data collecting devices 1110a, 1110b and uses the stored
time-series data of the measured values of the forward-and-backward-direction forces
to calculate the final alignment irregularity amount y
R. Accordingly, in addition to the effects explained in the first and second embodiments,
for example, the following effects are exhibited. That is, the data processing device
1120 can calculate the final alignment irregularity amount y
R at an arbitrary timing by reading the measured data at an arbitrary timing. Further,
the data processing device 1120 can output time-series variation of the final alignment
irregularity amount y
R at the same position. Further, the data processing device 1120 can output the final
alignment irregularity amounts y
R in a plurality of routes for each route.
<Modified example>
[0198] In the present embodiment, the case where the data collecting devices 1110a, 1110b
directly transmit the measured data to the data processing device 1120 has been explained
as an example. However, it is not always necessary to design as above. An inspection
system may be built by using cloud computing, for example.
[0199] Besides, also in the present embodiment, it is possible to employ the various modified
examples explained in the first and second embodiments.
[0200] Further, in the first and second embodiments, the case where the storage unit 501,
the data acquisition unit 502, the first frequency adjustment unit 503, the state
variable derivation unit 504, the second frequency adjustment unit 505, the track
state derivation unit 506, and the output unit 507 are included in one apparatus has
been explained as an example. However, it is not always necessary to design as above.
Functions of the storage unit 501, the data acquisition unit 502, the first frequency
adjustment unit 503, the state variable derivation unit 504, the second frequency
adjustment unit 505, the track state derivation unit 506, and the output unit 507
may be fabricated by a plurality of apparatuses. In this case, the inspection system
is constituted by using these plural apparatuses.
(Calculation examples)
[0201] Next, calculation examples will be explained. In the present calculation example,
derivation of a final alignment irregularity amount y
R based on the method of the first embodiment and derivation of a final alignment irregularity
amount y
R based on the method of the second embodiment were performed. In the method of the
first embodiment, when performing the data assimilation, the value to be normally
given as the measured value of the observation variable (fixed value) was set to 0
(zero). Further, in the method of the second embodiment, the forgetting factor c was
set to 0.9987.
[0202] Further, in contrast to the method of the first embodiment, derivation of a final
alignment irregularity amount y
R was performed based on a method in which as the values to be given as the measured
values of the observation variables (the measured values of the accelerations of the
vehicle body 11, the bogies 12a, 12b, and the wheel sets 13a to 13d in the right and
left direction), not the preset fixed value but the measured values are given as they
are (namely, the method described in Patent Literature 1).
[0203] Fig. 12 illustrates the present calculation example, and is a view illustrating the
curvature 1/R of the track 16 being the target of deriving the alignment irregularity
amount and the traveling velocity v of the railway vehicle. In Fig. 12, a graph 1201
indicates the traveling velocity of the railway vehicle, and a graph 1202 indicates
the curvature 1/R of the track 16. Note that the horizontal axis in Fig. 12 indicates
an elapsed time (second) from a reference time when the reference time is set to 0
(zero).
[0204] Each of Fig. 13A and Fig. 13B illustrates the present calculation example, and is
a view illustrating a distribution of eigenvalues of an autocorrelation matrix R.
Fig. 13A illustrates a distribution of eigenvalues of an autocorrelation matrix R
with respect to the forward-and-backward-direction force T
1 in the wheel set 13a, and Fig. 13B illustrates a distribution of eigenvalues of an
autocorrelation matrix R with respect to the forward-and-backward-direction force
T
2 in the wheel set 13b.
[0205] Fig. 14 illustrates the present calculation example, and is a view illustrating time-series
data of the measured values y of the forward-and-backward-direction forces T
1, T
2 and time-series data of predicted values y^
k of the forward-and-backward-direction forces T
1, T
2 (time-series data obtained by extracting low-frequency components included in the
time-series data of the measured values y of the forward-and-backward-direction forces).
In Fig. 14, the measured value indicates the time-series data of the measured value
y of the forward-and-backward-direction force, and bias indicates the time-series
data of the predicted value y^
k of the forward-and-backward-direction force. Note that the horizontal axis in Fig.
14 indicates a measuring time and a calculating time of the forward-and-backward-direction
forces T
1 to T
4, each of which is an elapsed time (second) from a reference time when the reference
time is set to 0 (zero).
[0206] Fig. 15 illustrates the present calculation example, and is a view illustrating the
time-series data of the high-frequency components of the forward-and-backward-direction
forces T
1, T
2. The time-series data of the high-frequency components of the forward-and-backward-direction
forces T
1, T
2 can be obtained by subtracting the time-series data of the predicted values y^
k of the forward-and-backward-direction forces T
1, T
2 from the time-series data of the measured values y of the forward-and-backward-direction
forces T
1, T
2 illustrated in Fig. 14. Note that the horizontal axis in Fig. 15 indicates an elapsed
time (second) from a reference time when the reference time is set to 0 (zero) and
indicates a calculating time of the time-series data of the high-frequency components
of the forward-and-backward-direction forces T
1, T
2.
[0207] Fig. 16A and Fig. 16B are views illustrating the alignment irregularity amounts y
R derived by the method of the first embodiment and the method described in Patent
Literature 1 by using the time-series data of the high-frequency components of the
forward-and-backward-direction forces T
1, T
2 illustrated in Fig. 15. In Fig. 16A, the calculated value indicates the alignment
irregularity amount y
R derived by the method described in Patent Literature 1, and the measured value indicates
the measured value of the alignment irregularity amount y
R. In Fig. 16B, the calculated value indicates the alignment irregularity amount y
R derived by the method of the first embodiment, and the measured value indicates the
measured value of the alignment irregularity amount yR. Here, as the calculated value
of the alignment irregularity amount y
R, an average value of the alignment irregularity amount y
R at the position of the wheel set 13a and the alignment irregularity amount y
R2 at the position of the wheel set 13b was used. Further, the measured value illustrated
in Fig. 16A and the measured value illustrated in Fig. 16B are the same. Note that
the horizontal axis in each of Fig. 16A and Fig. 16B indicates an elapsed time (second)
from a reference time when the reference
time is set to 0 (zero) and indicates a time corresponding to the position where the
alignment irregularity amount y
R exists. Further, in Fig. 16A, the illustration of data of a part at which a distance
from a starting point of the railway vehicle is small is omitted for convenience of
illustration.
[0208] Fig. 17A is a view illustrating the alignment irregularity amount y
R derived by the method of the second embodiment by using the time-series data of the
high-frequency components of the forward-and-backward-direction forces T
1, T
2 illustrated in Fig. 15. Fig. 17B is a view illustrating the alignment irregularity
amount y
R derived by the method described in Patent Literature 1 by using the time-series data
of the high-frequency components of the forward-and-backward-direction forces T
1, T
2 illustrated in Fig. 15. In Fig. 17A, the calculated value indicates the alignment
irregularity amount y
R derived by the method described in Patent Literature 1, and the measured value indicates
the measured value of the alignment irregularity amount y
R. In Fig. 17B, the calculated value indicates the alignment irregularity amount y
R derived by the method of the second embodiment, and the measured value indicates
the measured value of the alignment irregularity amount y
R. Here, as the calculated value of the alignment irregularity amount y
R, an average value of the alignment irregularity amount y
R1 at the position of the wheel set 13a and the alignment irregularity amount y
R2 at the position of the wheel set 13b was used. Further, the measured value illustrated
in Fig. 17A and the measured value illustrated in Fig. 17B are the same (these measured
values are also the same as the measured values illustrated in Fig. 16A and Fig. 16B).
Note that the horizontal axis in each of Fig. 17A and Fig. 17B indicates an elapsed
time (second) from a reference time when the reference time is set to 0 (zero) and
indicates a time corresponding to the position where the alignment irregularity amount
y
R exists. Further, in Fig. 17A and Fig. 17B, the illustration of data of a part at
which a distance from a starting point of the railway vehicle is small is omitted
for convenience of illustration.
[0209] When the calculated value in Fig. 16A and the calculated value in Fig. 16B are compared,
it can be understood that the alignment irregularity amount y
R derived by the method of the first embodiment matches the alignment irregularity
amount y
R derived by the method described in Patent Literature 1 with good accuracy. Further,
it can be understood that the calculated value and the measured value also match with
good accuracy. In like manner, when the calculated value in Fig. 17A and the calculated
value in Fig. 17B are compared, it can be understood that the alignment irregularity
amount y
R derived by the method of the second embodiment matches the alignment irregularity
amount y
R derived by the method described in Patent Literature 1 with good accuracy. Further,
it can be understood that the calculated value and the measured value also match with
good accuracy. Further, when the calculated value in Fig. 16B and the calculated value
in Fig. 17B are compared, it can be understood that the both values are almost the
same, and thus the equivalent alignment irregularity amount y
R can be derived by both the method of the first embodiment and the method of the second
embodiment.
(Another embodiment)
[0210] Note that the embodiments of the present invention explained above can be fabricated
by causing a computer to execute a program. Further, a computer-readable recording
medium in which the aforementioned program is recorded and a computer program product
such as the aforementioned program can also be applied as the embodiment of the present
invention. As the recording medium, it is possible to use a flexible disk, a hard
disk, an optical disk, a magneto-optic disk, a CD-ROM, a magnetic tape, a nonvolatile
memory card, a ROM, or the like, for example.
[0211] Further, the embodiments of the present invention explained above merely illustrate
concrete examples of implementing the present invention, and the technical scope of
the present invention is not to be construed in a restrictive manner by these embodiments.
That is, the present invention may be implemented in various forms without departing
from the technical spirit or main features thereof.
[0212] Note that the entire contents of the description and drawings of Patent Literature
1 can be incorporated herein by reference.
INDUSTRIAL APPLICABILITY
[0213] The present invention can be utilized for inspecting railway vehicles, for example.