Field of the Invention
[0001] A device for traversing of yarn wound-up on a spool fitted into the workplace of
a textile machine comprising a longitudinal traversing rod common for multiple workplaces
and coupled with a drive imparting straight reverse motion to it and a controlling
system determining the position of the rod dead points, whereas the longitudinal traversing
rod is parallel with a longitudinal winding shaft intended for numerous workplaces,
further comprising at least two magnetic pairs, one of the magnets of which is always
located on the frame of the machine, whereas the other magnet is located on the traversing
rod.
Background art
[0002] With textile machines, e.g. open end spinning machines, spooling or two-for-one twisting
machines, the traversing of yarn at spool winding is commonly performed by means of
a through traversing rod passing along one side of the machine's workplaces. With
numerous workplaces lined up in rows the traversing rod is as long as 50 metres for
instance, which means its weight is substantially high.
[0003] Cross-wound cylindrical or conical spools roll off their wound-up surface against
winding rollers, the rotation axis of which is parallel to the axis of the traversing
rod and the traversing rod performs straight reverse motion, its travel matching the
length of the surface line of the wound spool's package. Regarding the productivity
of the machine, the velocity of the yarn driven to the wound-up spool is high, which
requires a high frequency of the straight reverse motion of the traversing rod.
[0004] From the point of view of producing the cross-wound build, it would be desirable
the curve of the traversing rod motion to be saw-like, i.e. the velocity of the traversing
rod to be constant and to change in step at dead points to reach the same velocity
of the opposite sense.
[0005] In practice, it is not possible to achieve the ideal state mainly due to the big
inertial mass of the traversing rod. The rod's deceleration and acceleration at dead
points is limited, the change of the sense of velocity at dead points takes some necessary
time. Within that period of time the yarn is not deposited onto the spool in a screw
line upon a pitch producing the required cross-wound build, but the pitch decreases
to zero at the dead point and the individual yarn coils are deposited onto each other.
The yarn accumulates in those spots of the spool and the diameter of the build increases
faster locally.
[0006] That is prevented by the modification of the motion of the traversing rod at dead
points. With one common solution the travel remains constant and the position of both
dead points slowly shifts in one and the other direction concurrently. With another
usual solution the size of the travel changes and the positions of the dead points
mutually shift in an opposite sense, by means of which the size of the travel increases
and decreases in turns. From the point of view of the quality of the build the second
solution is more advantageous, although it is not easy to implement with a cam mechanism
drive or a mechanism where the servomotor does not change the sense of rotation.
[0007] At the time of the motion of the rod at a constant velocity the necessary output
of its driving unit is relatively small as it only makes for overruling passive resistances
and deflecting yarns. However, at dead points significant alterations of the output
of the driving unit occur, firstly by reason of detracting and subsequently imparting
inertia to the mass of the traversing rod. With the first method employing a constant-travel
motion, a cam mechanism is usually used and the energy accumulates in the rotation
energy of the drive mechanism. With the second method, where the motor performs a
reverse motion, the problem is solved either by means of a big nominal driving torque
of the servomotor and/or the accumulation of the kinetic energy produced at braking
of the inertial mass of the traversing rod before the dead point and a reverse release
of the energy accumulated at starting the traversing rod after the dead point. However,
the moment of inertia of servomotors with big driving torques is big and it increases
the total reduced moving mass, thus the achievable increase in the acceleration of
the rod is little or none.
[0008] Another problem besides the provision of the required shape of the spool's build
edges is the production of concurrently deposited bands of coils of yarn located close
to each other at augmenting the diameter of the wound-up spool. At augmenting the
diameter of the spool the axial position of individual successively laid coils of
yarn, which near and recede from each other in turns, gradually changes. At the time
of nearing the coils, bands are periodically produced breaking the shape of the build
and complicating the progress of winding. That is prevented by gradual changes to
the frequence of motion of the traversing rod based on certain prescriptions.
[0009] Current solutions of traversing rod drives usually employ cam mechanisms. A first
mechanism of a constant travel provides the basic approximately saw-like travel of
the traversing rod including velocity changes at dead points. The second superimposed
mechanism makes for slow concurrent shifts of the dead points. Both mechanisms are
loaded by a total force necessary to induce the motion of the rod. The dissolution
of the bands is performed either by means of a controlled variator usually driven
by another cam mechanism, or including a frequency converter into the power supply
circuit of the driving electric motor. The traversing box comprising those mechanisms
is placed on only one of the sides of the machine, thus the long traversing rod is
sensitive to production of vibrations. It spreads not only longitudinal waves of deformations,
but transverse waves as well, caused by buckling stress of the rod and its deflection
from the guide bearings. Furthermore, the deflection results in the increase of frictional
forces. Compared to the longitudinal waves, the transverse waves on the rod are of
lower velocity and the resulting oscillation of the rod is usually very complex. The
motion of the free end of the traversing rod thus differs from the motion of its part
located close to the drive mechanism.
[0010] It is obvious that the main reason limiting the traversing velocity and complicating
the action of the drive mechanism of the traversing rod are the inertia forces at
dead points produced as a result of insufficient compensation of the effects of substantive
decelerations and accelerations of the moving masses.
[0011] Some devices based on the prior art use springs-to absorb the energy of the moving
mass forces. It is advantageous such spring to have non-linear characteristic, matching
the force necessary to achieve the required motion of the rod much better. With mechanical
or pneumatic springs the provision of such parameters is difficult. In some cases,
rubber or plastic bumpers acting on the traversing rod in the area of its dead points
are used to load off the cam mechanisms. However, such springs cause strokes and oscillations
of the rod and their service life is rather low.
[0012] Furthermore, those devices usually do not allow setting the travel of the traversing
rod and thus changing the width of the build on the spool. The traversing rod is stressed
by big compression forces requiring a respective increase of the cross-section of
the rod, which results in subsequent increase in the weight of the traversing rod
and thus increasing undesirable inertia forces. Even with substantial cross-sections
of the traversing rod the oscillation usually results in a different course of the
travel of the rod on different spots of the machine.
[0013] Another option is to perform braking and start-ups of the traversing rod by means
of magnets. Their advantage is based on their effect to a theoretically infinite distance
as well as the smooth course of the dependence of the force value on distance, the
result of which is the stroke-free effect on the traversing rod. As another advantage,
there is the strongly non-linear dependence of the force value on distance (approximately
at mat cube), significantly contributing to dampening the vibrations and resonance
elimination. As far as the construction and economic point of view is considered,
it is more advantageous to use permanent magnets instead of electromagnets. The solution
according to CZ PV 2007-214 is schematically presented in Fig. 1. Two pairs of magnets
101-201 and
102 - 202 are used within it, the first magnets
101, 102 of both pairs of magnets are placed in an adjustable way on the machine frame
100 and spaced mutually. The second magnets
201, 202 of both pairs of magnets are fixed to the traversing rod
200 placed in the machine frame
100 by means of a guide
10. At the traversing motion of the rod
200 the magnet
201, 202 fixed to the traversing rod
200 approximates and recedes the magnet
101, 102 placed on the machine frame
100 in turns, the same poles of the magnets of each cooperating pair are directed towards
each other. At the approximation of the magnets of one pair, the magnets repel each
other, the maximum repelling force matching the least mutual distance of the magnets'
fronts achieved at the traversing rod's dead points. The minimum distance is set by
means of shifting the magnet located on the machine frame, which is performed by axial
servomotors not represented in the figure.
[0014] The magnets' repelling force value is selected based on the type of the wound-up
yarn considering its thickness and flexibility. Thereat, it is necessary to respect
the thermal expandability of the rod, the resistances acting against the motion of
the rod and, of course, the operation of the superimposed mechanism controlling the
shifts of the traversing rod's dead points by reason of overlaying the edges of the
build. Thus, setting the mutual minimum distance of the magnets of one pair, which
is a value of tenths of millimetres, and fixing the adjusting magnet against the machine
frame require a high level of accuracy. However, it is not commonly achieved with
solutions according to the prior art.
[0015] Another disadvantage of placing the magnets according to CZ PV 2007-214 is the fact
that the magnets attenuate the longitudinal oscillation of the traversing rod only
with motions in direction away from the drive mechanism of the rod for traversing.
Even though such attenuation is significant as it is performed at the moment of the
traversing rod is disadvantageously buckle-stressed and the aim of CZ PV 2007-214
is achieving exactly that effect, the absence of attenuation of the longitudinal oscillation
of the traversing rod at its motion in the opposite direction proves that the solution
is not ideal as all sources of vibrations, noise and increased loading and wear have
not been completely dealt with.
[0016] The aim of the invention is to remove or at least significantly reduce the insufficiencies
of the prior art and to achieve a decrease in vibrations, noise and wear and achieve
higher operational parameters of the traversing mechanism and thus the machine as
a whole by means of attenuating the longitudinal vibrations of the rod's motion towards
the drive mechanism of the traversing rod as well.
Principle of the Invention
[0017] The aim of the invention is achieved by means of a device for traversing the yarn
wound-up on a spool deposited in the winding system of a textile machine's workplace,
which comprises at least two magnetic pairs, each of which includes mutually repelling
magnetic poles, one of which is always located on the machine frame, the other is
located on the traversing rod, the principle of which is based on the fact that at
least two magnetic pairs are located in the area of the traversing rod's free end.
Even at a travel, at which the traversing rod is being pulled, the longitudinal oscillation
of parts of the traversing rod's free end is virtually attenuated with such arrangement.
[0018] Considering constructional simplifications, the magnetic pairs may include two fixed
magnets secured in a way allowing rearrangement to the machine frame and at least
one common moving magnet fastened to the traversing rod.
[0019] In a different application, each magnetic pair comprises a fixed magnet fastened
in a way allowing rearrangement to the machine frame and one magnet secured to the
traversing rod.
[0020] In another application, the device includes three magnetic pairs, one of which is
located in the area of the traversing rod's end connected to the traversing box. By
means of such arrangement the tension in the traversing rod in the area of the right
dead point can be influenced.
[0021] It is advantageous to fasten the fixed magnets to the machine frame in an adjustable
way by means of servomotors fastened to the frame, the output of the servomotors is
a straight shift of the fixed magnets along the traversing rod, the output member
of the servomotor is fixed to the frame after performing the straight shift. Thereat,
it is especially advantageous to couple the servomotors of the fixed magnets with
the control unit determining the position of the traversing rod's dead points. That
way, computer control of the traversing system is enabled.
[0022] At least one of the magnetic pairs is formed by a pair of Halbach arrays. The major
advantage of the device according to the invention is the significant weight reduction
of the arrangement of magnets compared to bipolar magnets, which is particularly important
with magnets fastened to the traversing rod and participating in the value of its
inertial mass.
Description of the drawing
[0023] The exemplary applications of the device according to the invention are schematically
demonstrated in the drawings. For illustrative purposes, Fig. 1 shows the device according
to the prior art, Fig. 2a and 2b show two alternative priority designs of the device
according to the invention, Fig. 3 shows another design of the device according to
the invention, Fig. 4 shows the course of the velocity of the start and end of the
traversing rod with the device according to the prior art and Fig. 5 shows a comparison
of the courses of the longitudinal position of the start and the end of the traversing
rod with a device according to the prior art and according to the invention.
Examples of embodiment
[0024] In the frame
1 of a textile machine designed according to Fig. 2a the traversing rod
2 is arranged by means of a guide
10. In the exemplary application, the traversing rod
2 is driven by means of a not represented crank or cam mechanism arranged in the traversing
box
3. The mechanism transforms the rotational motion of the driving motor's output shaft
to straight reverse motion of the traversing rod
2. An alternative application uses a linear driving servomotor.
[0025] In the free end area of the traversing rod
2 there are moving magnets
21 and
22, firmly fastened to the traversing rod
2. On the machine frame
1 are arranged fixed magnets
11 and
12 in a way allowing their sliding. The magnets are disc-shaped with a central opening
and they are arranged coaxially with the traversing rod
2. The traversing rod 2 passes through the openings of the fixed magnets
11, 12 freely. With another not represented mutual ordering the magnets are arranged outside
the traversing rod. The moving magnet
21 and the fixed magnet
11 and the moving magnet
22 and the fixed magnet
12 form cooperating magnetic pairs. The magnets of each pair
11 - 21, 12 - 22 are directed towards each other with their opposite poles so that they repel each
other. The fixed magnets
11, 12 are adjustable against the frame, whereas are fixed in positions so that the difference
of the
L1 distance of nearing poles of fixed magnets
11, 12 and the
L2 distance of reverse poles of moving magnets
21, 22 fixed to the traversing rod
2 is equal to the sum of the travel of the traversing rod
2 and the required clearances remaining between the nearing poles of one and the other
pair of magnets
11 - 21, 12 - 22 at the left and right dead point of the traversing
rod 2 and preventing mutual contacts of the magnets of each pair.
[0026] With the design shown in Fig. 2b the two magnetic pairs are formed from a single
moving magnet
20, replacing two moving magnets
21, 22, and of two fixed magnets
11, 12.
[0027] With the design shown in Fig. 3 the device according to the invention includes another
pair of magnets comprising a moving magnet
23 fixed on the traversing rod
2 and a fixed magnet
13 located in a way allowing its slide on the machine frame
1, placed close to the traversing box
3. The fixed magnet
13 is adjusted against the frame so that the required clearances as mentioned above
are present between the nearing poles of pairs of magnets
13 - 23 and
12 - 22 at the right dead point of the traversing rod
2. Those might be slightly different, whereby the tension in the traversing rod in the
area of the right dead point can be influenced.
[0028] In an example of embodiment the magnets
11, 12, 13, 21, 22, 23 are standard bipolar permanent magnets, in another example of embodiment are multi-polar
and forming a Halbach array. Not demonstrated servomotors generally known to those
skilled in the art are advantageously used for readjusting fixed magnets
11, 12, 13 against the machine frame 1, while the servomotors are stabilized after adjusting
the position of the fixed magnets.
[0029] The servomotors of fixed magnets
11, 12, 13 are advantageously coupled with a not demonstrated control unit, used for controlling
the positions of the dead points of the traversing rod
2. Furthermore, the device may include sensors of the axial position of the traversing
rod
2 or sensors of the value of the repelling force, which are also not demonstrated.
[0030] Fig. 4 shows the course of velocity
v of parts of the traversing rod
200 with the device according to the prior art. The lighter curve
v1 is the course of the velocity of parts of the traversing rod
200 on the spot
203 of coupling with the traversing box
300 and the darker curve
v2 is the course of the velocity of parts of the traversing rod
200 on the spot
204 the free end of the traversing rod
200. At travel
z1 the traversing rod
200 is pushed (it moves from the left to the right dead point), at travel
z2 the traversing rod
200 is pulled (it moves from the right to the left dead point). It is clear that when
the traversing rod
200 is pushed, its longitudinal oscillation is significantly reduced. On the contrary,
at reverse motion, at which the traversing rod
200 is pulled, major longitudinal vibrations occur.
[0031] By analogy with Fig. 4, the upper part of Fig. 5 shows the course
ps of parts of the traversing rod
200 on the spot
203 of coupling with the traversing box
300 and the spot
204 at the free end of the traversing rod
200 with a device according to the prior art based on Fig. 1, and the lower part of it
shows the course
pv of parts of the traversing rod
2 on the spot
24 of coupling with the traversing box
3 and on the spot
25 at the free end of the traversing rod
2 with a device according to the invention based on Fig. 2 and 3. It is clear that
the longitudinal oscillation of parts of the traversing rod
2 on spot
25 at the free end of the traversing rod
2 is virtually dampened even with travel
z2, at which the traversing rod
2 is pulled.
[0032] Compared to the mentioned exemplary applications according to the invention the design
according to Fig. 2 is more advantageous than the design according to Fig. 3. The
lower number of magnets results in a lower weight of the traversing rod
2 and further reduction of costs for each pair of magnets
13-23 and the respective axial servomotor for shifting the fixed magnet
13. The arrangement of magnets according to Fig. 2a, 2b is advantageously used when the
motion of the traversing rod
2 generated by the traversing box
3 is smooth, i.e. without strokes, when the part of the traversing rod
2 near the traversing box
3 is sufficiently stiff and when there is no requirement for dividing the dampening
between two pairs of magnets
12 - 22 and
13 - 23 with the same sense of the dampening effect.
[0033] Compared to the arrangement according to Fig. 2, the arrangement according to Fig.
3 may meet more universal requirements, especially due to the fact that it allows
to influence the forces acting on both ends of the traversing rod
2 by means of different distances of magnets
12 - 22 and
13 - 23 and to achieve the occurrence of even tensile stress in the traversing rod
2. By means of combining the forces of magnets
12 - 22 and
13 - 23, the distances of which are different, the course of the resulting force can be changed
and adapted to the force necessary for starting and braking the traversing rod
2.
List of reference marks
[0034]
- 1
- machine frame
- 10
- traversing rod lead
- 11
- fixed magnet
- 12
- fixed magnet
- 13
- fixed magnet
- 2
- traversing rod
- 20
- common moving magnet
- 21
- moving magnet
- 22
- moving magnet
- 23
- moving magnet
- 24
- area on traversing rod close to traversing box
- 25
- area on traversing rod at its loose end
- 3
- traversing box
- 100
- machine frame (prior art)
- 101
- fixed magnet ( " - ")
- 102
- fixed magnet ( " - ")
- 200
- traversing rod ( " - ")
- 201
- moving magnet ( " - ")
- 202
- moving magnet ( " - ")
- 203
- area on traversing rod close to traversing box ( " - ")
- 204
- area on traversing rod at its loose end ( " - ")
- 300
- traversing box ( " - ")
- L1
- distance (of nearing fixed magnets fronts)
- L2
- distance (of reverse moving magnets fronts)
- ps
- position course of spots 203 and 204 of the traversing rod (according to prior art)
- pv
- position course of spots 24 and 25 of the traversing rod (according to invention)
- v1
- velocity course of traversing rod spot 203 (according to prior art)
- v2
- velocity course of traversing rod spot 204 (according to invention)
- z1
- traversing rod travel period of the traversing rod being pushed
- z2
- traversing rod travel period of the traversing rod being pulled
1. A device for traversing of yarn wound-up on a spool fitted in a winding system of
a textile machine's workplace, comprises a longitudinal traversing rod (2) common
for numerous workplaces and coupled with a drive providing it with longitudinal reverse
motion and a controlling mechanism determining the position of the dead points of
the traversing rod (2), whereas the longitudinal traversing rod (2) is parallel to
the longitudinal winding shaft intended for numerous workplaces, whereas further comprising
at least two magnetic pairs each of which comprises repelling poles of magnets (11,
21; 12, 22; 11, 20; 12, 20), of which one magnet (11, 12) is always located on the
machine frame (1) and the other magnet (21, 22, 20) is located on the traversing rod
(2), characterized in that, the at least two magnetic pairs (11, 21; 12, 22; 11, 20; 12, 20) are located in the area
of the free end of the traversing rod (2).
2. A device according to claim 1, characterized in that, the two magnetic pairs comprise two fixed magnets (11, 12) fastened to the machine frame
(1) in an adjustable way, and at least one common moving magnet (20) fastened to the
traversing rod (2)..
3. A device according to claim 1 or 2, characterized in that, the each magnetic pair comprises a fixed magnet (11, 12) fastened to the machine frame
(1) in an adjustable way and one magnet (21, 22) fastened to the traversing rod (2).
4. A device according to any of claims 1 to 3, characterized in that, the comprises three magnetic pairs (11, 21; 12, 22; 13; 23), of which one magnetic pair
(13, 23) is located in the area of the end of the traversing rod (2) coupled with
the traversing box (3).
5. A device according to any of claims 1 to 4, characterized in that, the fixed magnets (11, 12, 13) are placed on the machine frame (1) in an adjustable way
by means of servomotors fastened to the frame (1), whereas the output of the servomotors
is the linear shift of the fixed magnets (11, 12, 13) along the traversing rod (2),
whereas after performing the linear shift the output member of the servomotor is fixed
to the frame (1).
6. A device according to claim 5, characterized in that, the servomotors of the fixed magnets (11, 12, 13) are coupled with the control unit determining
the position of the dead points of the traversing rod (2).
7. A device according to any of claims 1, 3 to 6, characterized in that, the at least one of the magnetic pairs (11, 21; 12, 22; 13; 23) is formed by Halbach
arrays.