[0001] The present invention relates to an implement for bending metal plates or sheets,
known under the name V block, and more in particular to the shape of the lead-in curve
of implements of this type.
[0002] The known V blocks mainly consist of one solid piece, having at least one flat side,
in which a straight, elongated recess is provided whose profile over the entire length
is identical and V-shaped. The shape of said recess is moreover preferably symmetrical
with respect to a plane extending in its longitudinal direction, which is perpendicular
to the flat topside of the V block (hereinafter called the plane of symmetry of the
recess).
[0003] The flat topside of the V block merges into the flanks of the recess via roundings.
Said roundings have a profile whose radius of curvature is identical at every point.
The profile of said roundings is designated by the name "lead-in curve".
[0004] Below the lead-in curve, the flanks are constructed to be planar and converge in
a downward direction, and they meet where they form the lowest part of the recess.
The lead-in curve is thus a curve whose start adjoins the flat side of the V block
and whose end adjoins one of the flanks of the recess.
[0005] The profile of the V-shaped recess is likewise rounded below, where the two flanks
merge into one another.
[0006] An important characteristic of a V block consists of the so-called V value which
on the profile of the recess represents the following distance: "the distance between
the intersections of, on the one hand, the straight lines coinciding with the rectilinear
portion of each flank of the recess and, on the other hand, the straight line coinciding
with the flat topside of the V block, measured along the last mentioned straight line".
[0007] Another characteristic of a V block consists of the value of the angle between the
flanks of the V-shaped recess. This is the angle - on the profile of the recess -
between the straight lines coinciding with the rectilinear portion of each flank,
measured between those portions of said straight lines which extend from the intersection
towards the topside of the recess.
[0008] The known V blocks are constructed in such a way that the lateral edges run parallel
with the plane of symmetry of the recess, and the front side and rear side - into
which the recess opens - are perpendicular to said plane of symmetry and to the topside.
The following will show that the length of the V block and thus of the recess determines
the length of the bend which can be achieved with the aid of this implement. The width
of the V block is only slightly less than the width of the recess and the lead-in
curves situated on both sides thereof.
[0009] Bending of a plate or sheet, with the aid of a V block, is effected as follows. The
plate or sheet is positioned on the flat topside of the V block in such a way that
the imaginary line on the plate or sheet, where the bend is to be achieved, coincides
with the plane of symmetry of the recess. Said line which in the following is called
the bending line must not be longer, in this case, than the length of the V-shaped
recess.
[0010] Bending itself is effected by means of a pressure implement or ram arranged above
the V block. This pressure implement has a narrow rectilinear underside having a virtually
constant width and a length which is at least equal to the length of the bending line.
Said pressure implement is positioned in such a way that said underside extends along
the length of the recess and is parallel to the flat topside of the V block, the centre
line of said underside being situated in the plane of symmetry of the recess.
[0011] The pressure implement is furthermore positioned on means which are able to move
said implement vertically up and down and which, inter alia, are designed in such
a way that, if the pressure implement is moved to the topside of a plate or sheet,
a sufficient downward force can be generated to bend said plate or sheet. During the
movements of the pressure implement the position indicated hereinabove with regard
to the recess in the V block is maintained at all times.
[0012] After the plate or sheet has been correctly positioned, the pressure implement is
moved, from a position where its underside is positioned above the plate or sheet,
downward as far as the plate or sheet. It follows from the above that, as this happens,
the longitudinal axis of the underside of the pressure implement coincides with the
bending line.
[0013] By means of the pressure implement, a downward force is then exerted on the plate
or sheet, abreast of the bending line which is located above the recess, and where
the plate or sheet is thus not supported. The plate or sheet rests, on both sides
of the recess, on the flat side of the V block. As a result of this downward force
there are produced, abreast of said two supporting surfaces, upward reaction forces
which, owing to the symmetrical positioning, form two identical but opposite moments
with the downward force.
[0014] Said bending moments ensure that the plate or sheet is bent symmetrically. As the
pressure implement continues to move downwards in the recess, the plate or sheet is
bent further.
[0015] From the instant where the bend begins to form in the plate or sheet, the plate or
sheet rests on the lead-in curves. As the plate or sheet bends further, said support
surface is positioned further and further down on the lead-in curves.
[0016] The pressure implement is finally moved into such a position, that the desired bending
angle in the plate or sheet has been obtained. The term bending angle here refers
to the angle which is formed between the portions of a plate or sheet, which are situated
on each side of the bending line. In the case of a bent plate or sheet this is the
angle (< 180°) which is formed between the angle-forming portions of the plate or
sheet (this, on a cross-section, is the angle (< 180°) between the straight lines
coinciding with the rectilinear portions of the plate or sheet on each side of the
bend). In the case of a flat plate or sheet, the "bending angle" is equal to 180°.
[0017] For further explanation of the problem on which this invention is based we refer
to the accompanying Figures in which:
Figure 1 represents a vertical cross-section of a V block, on which a bent plate or
sheet is presented at two different bending angles;
Figure 2 shows, in graphic form, the size of the force exerted by the plate or sheet
on the V block (according to the prior art) as a function of the bending angle of
said plate or sheet;
Figure 3 presents, in graphic form, the size of the contact pressure arising between
plate or sheet and V block - according to the prior art - as a function of the bending
angle of the plate or sheet;
Figure 4 presents, in graphic form, the ratio "slip speed/rolling speed" as a function
of the bending angle of the plate or sheet, for a V block according to the prior art;
Figure 5 presents, in graphic form, the wear of a V block according to the prior art
as a function of the bending angle of the plate or sheet.
[0018] Figure 1 presents, in vectorial form, the forces (F, F1, F2, R1, R2, F', F'1, F'2,
R'1, R'2) acting on the plate or sheet (3) and on the V block (1) at the instant that
the pressure implement (not shown) exerts a force (F) on the plate or sheet (3).
[0019] In the case of the V block (1) from Figure 1, according to the prior art the radius
of curvature (ρ
j) of the lead-in curves (2) is constant.
[0020] In the course of bending a plate or sheet (3), the pressure implement (not shown)
exerts a vertical force (F) in the centre of the plate or sheet. At a certain time,
said plate or sheet (3) has attained a bending angle (j1) (the topmost situation of
the plate or sheet on Figure 1). The plate or sheet (3) is supported abreast of the
points (4) by the roundings (2) of the V block (1). The vertical force (F) gives rise
to two forces (F1, F2) on the V block (1), as a result of which two reaction forces
(R1, R2) opposite thereto are produced, each of which act, with the same respective
force, on the plate or sheet (3) in one of the support points (4). Said forces (F1,
F2) and said reaction forces (R1, R2) have a direction perpendicular to the plate
or sheet (3) and a magnitude so as to be able to form, together with the vertical
force (F), a closed triangle of forces. Their projection on a vertical, in other words,
must be equal to half the force (F).
[0021] Owing to the forces (F1, F2) abreast of the support points (4), the material of the
V block (1) is indented slightly, so that as a matter of fact one has to talk in terms
of support surfaces, abreast of the points (4).
[0022] Owing to the opposite moments which are formed, on the one hand, by the forces (F2)
and (R2) and, on the other hand, by the forces (F1) and (R1), the plate or sheet (3)
is bent.
[0023] At a later time, the plate or sheet (3) encounters a situation where the bending
angle (j2) has been achieved (the lowermost situation of the plate or sheet in Figure
1). The plate or sheet (3) is now supported, abreast of the points (5) lower than
the points (4), by the roundings (2). The vertical force (F') which is of the same
size as the force (F) now gives rise, in the same manner as described above for bending
angle (jl), to forces (F'1, F'2) and reaction forces (R'1, R'2), directed perpendicular
to the plate or sheet (3). As can be ascertained in Figure 1, after comparing the
magnitude of the forces (F1, F2, R1, R2) at bending angle (j1) and (F'1, F'2, R'1,
R'2) at bending angle (j2), said respective forces are larger at bending angle (j2).
[0024] The accompanying Figure 2 shows the course of a reaction force (R1), (R2) as a function
of the bending angle (j). The reaction force (R1), (R2) is expressed in [N/mm], being
the reaction force (in Newtons) per mm in length of the plate or sheet which rests
on the lead-in curve.
[0025] The accompanying Figure 3 shows the course of the contact pressure (σ
j) (between plate or sheet (3) and lead-in curve (2)) as a function of the bending
angle (j). Said contact pressure is directly proportional to the square root of the
forces (F1), (F2). It is the force per unit surface of the contact area abreast of
point (5).
[0026] The wear (We
j) of the V block can be calculated mathematically with the aid of the formula:

[0027] The slip speed at a certain point of the lead-in curve (function of the bending angle
(j)) is the speed at which the plate or sheet moves in a direction tangential to the
lead-in curve at that point. This is the speed of the pressure implement (dY
j) multiplied with the sine of the angle (⌀) between the straight line according to
the travelling direction of the pressure implement and the straight line perpendicular
to the rounding.
[0028] The rolling speed at a certain point of the lead-in curve is the speed with which
a point of the plate or sheet moves as a result of rolling over the lead-in curve
at that point. This is therefore the radius of curvature (ρ
j) at that point, multiplied with the angular speed (dρ
j). The ratio between slip speed and rolling speed was calculated mathematically and
plotted, as a function of the bending angle (j), in Figure 4. By applying the abovementioned
formula for calculating the wear, Figure 5 is obtained, where the wear of the V block
is plotted as a function of the bending angle (j) of the plate or sheet (3).
[0029] From the above it is thus clear that, as the bending angle (j1, j2) decreases, greater
wear (Wej) of the V block (1) arises, and the contact pressure between plate or sheet
(3) and V block (1) increases up to considerable magnitudes. On the other hand, in
the case of the known V blocks, the plate or sheet will slide more than it will roll
over the roundings (2).
[0030] The high wear (Wej) of the V block (1) abreast of the roundings (2) as a result of
the high contact pressure (σj) and high slip speed is a major drawback of the known
V blocks. Another drawback is that, as a result of the high contact pressure (σj)
an imprint is formed in the bent plate or sheet (3). Still another drawback consists
in the fact that permanent markings on that plate or sheet (3) are produced, owing
to the plate or sheet (3) sliding over the roundings (2) more than it rolls.
[0031] The object of the invention is to overcome the abovementioned drawbacks by providing
a V block, whose wear is reduced and by means of which - if the V value of the V block
is chosen correctly - plates or sheets can be bent without causing imprints or marks
thereon. For the sake of clarity of the following description, reference is made to
the V block (1) from Figure 1, under the assumption that the radius of curvature (ρj)
corresponds to the characterizing features of the invention.
[0032] According to the invention, a V block (1) is then presented for bending plates or
sheets (3), consisting of a solid piece having at least one flat side (8), which via
roundings (2) merges into the flanks (6) of an elongated recess (7) having a V-shaped
profile which is provided in said flat side (8), while the profile of the recess (7)
and of said roundings (2) is identical over their entire length, characterized in
that the roundings in profile have a lead-in curve (2) whose radius of curvature (ρ)
adopts at least two different values, and in that at at least one point on the lead-in
curve (2) the radius of curvature (ρ) is greater than the radius of curvature (ρi)
of the start of the lead-in curve - where it merges into the flat side (8) of the
V block (1).
[0033] The advantage of a V block of this type is that it reduces the imprint of the plate
or sheet at too high a contact pressure (σj).
[0034] During bending of a plate or sheet there is exerted, namely, at the point where the
plate or sheet (3) is in contact with the rounded transitions (2) between flat side
(8) and flanks (6) of the recess (7), a force by said plate or sheet on the lead-in
curves, which produces a small deformation of the material of the V block. As a result
there is formed, instead of a contact line, a contact area whose area is directly
proportional to the radius of curvature of the lead-in curves (2) at that point. A
greater radius of curvature (ρj) consequently results, for the same force, in a smaller
contact pressure (σj) (force per unit surface). In order to reduce or avoid the imprint
in the plate (3), the radius of curvature (ρj) must be such, on at least one point
of the lead-in curve (2), that at that point where in the case of the intended use
too large a force is exerted, it has a value which is greater than the radius of curvature
(ρi) of the start of the lead-in curve (2), so that said contact area is sufficiently
large to reduce the contact pressure (σj) or to keep it below the value at which imprinting
is obtained in the plate or sheet to be bent (for the correct choice of the V value
of the V block). By limiting the contact pressure (σj) the wear (Wej) of the V block
according to the invention is likewise limited.
[0035] A particularly advantageous embodiment of this invention is obtained by giving the
rounded transitions (2) between flat side (8) and flanks (6) of the V-shaped recess
(7) a profile which is defined by a curve whose various values of the radius of curvature
(ρj) increase from the flat side (8) towards the flank (6) of the recess (7).
[0036] In an embodiment of this type, according to the invention, the problem of imprinting
of the plate - at too high a contact pressure (σj) - is overcome in an even more efficient
way.
[0037] After all, during bending of a plate or sheet, as described for the application of
the known V blocks, an increasing force (F'1 > F1; F'2 > F2) is observed on the roundings
(2), as the plate or sheet (3) is given a smaller bending angle (j2 < j1). Since a
smaller bending angle corresponds to a contact area between plate or sheet (3) and
V block (1), which is situated lower down on said roundings (2), the abovementioned
problem is overcome in a particularly efficient manner by letting the various values
of the radius of curvature (ρj) of the profile of said roundings (2) increase in the
direction of the flank (6) of the recess (7).
[0038] A further advantage of a V block having a radius of curvature (ρj) of the roundings
(2), which increases in a downward direction, consists in the plate or sheet rolling
over the rounding to a greater extent than was the case for the roundings which do
not have such a feature.
[0039] This advantage, combined with the advantage of the contact pressure (σj) kept within
limits has the following associated advantages: namely, that the V block (1) will
be subject to less wear (Wej), and that any marking on the plate (owing to slipping
in combination with a high contact pressure) will be avoided.
[0040] The drawbacks of the known V blocks are overcome in an even more efficient manner
by ensuring for a V block (1) having an angle β that the ratio of the radius of curvature
(ρe) of the end of the profile of the rounding (2) - where it merges into a flank
(6) of the recess (7) - with respect to the radius of curvature (ρi) of the start
of the profile of the rounding (2) - where it merges into the flat side (8) of the
V block (1) - is within the limits defined by the following formulae:
Lower limit:

Upper limit:

[0041] If, however, within the abovementioned limits the following ratio is employed:

the described drawbacks are reduced to an absolute minimum.
[0042] The most advantageous course of the lead-in curve (2), in the light of the drawbacks
to be overcome, is achieved, however, if the lead-in curve (2) has the coordinates
defined by the following equations, in a rectangular set of x-y axes having its origin
in the starting point of the curve (where it merges into the flat side (8) of the
V block) and having a horizontal X axis in the extension of that flat side (8), and
directed towards the other lead-in curve (2), and having a vertical, upwards-directed
Y axis


with 0 ≦ φ ≦ 90°-β/2 (β > 0°)
in which:
- m is a constant value from 1.1 to 1.5 inclusive,
- φ is the angle, varying from 0 to 90°-β/2, which is formed between the Y axis and
the straight line perpendicular to the rounding
- α = tan⁻¹ (m)
- β is the angle of the V block
- ρi is the radius of curvature of the start of the curve.
A curve of this type is denoted with the name "logarithmic spiral".
[0043] The optimum course of the lead-in curve is obtained if in the abovementioned equations
m = 1.2.
[0044] For practical reasons, however, preference is given to an approximation of this optimal
lead-in curve. This involves composing the lead-in curve from a number of successive
portions having a constant radius of curvature (sections of a circle). The greater
the number of portions into which the lead-in curve is subdivided, the better, obviously,
the approximation.
[0045] The coordinates of starting and end point of each portion are defined according to
the abovementioned equations for the (x, y) coordinates.
[0046] The value of the radius of curvature is defined according to the following equation:

in which:
- xi+1:
- is the x coordinate of the end point of a particular portion of the lead-in curve
- xi:
- is the x coordinate of the starting point of that portion
- φi+1:
- is the value of the angle φ for the end point of that portion of the lead-in curve
- φi:
- is the value of the angle φ for the starting point of that portion of the lead-in
curve
The coordinates (x
c, y
c) of the centre of curvature of each portion are defined according to the following
equations:


[0047] In the following, the advantages are discussed in more detail, and a number of examples
of possible embodiments according to the invention are provided.
[0048] In doing so, reference is made to the accompanying Figures in which:
Figure 6 indicates how the radius of curvature (ρj) of the lead-in curve varies as
a function of the bending angle (j) of the plate or sheet, for a possible embodiment
of a V block according to the invention;
Figure 7, for a V block according to Figure 6, indicates how the reaction force (Rj)
increases as a function of the bending angle (j) of the plate or sheet;
Figure 8 represents the variation in contact pressure (σj) as a function of the bending
angle (j);
Figure 9 represents the variation in ratio slip speed/rolling speed as a function
of the bending angle (j);
Figure 10 represents the variation in wear (in Newtons per mm²) as a function of the
bending angle (j);
Figure 11 depicts a lead-in curve of a V block according to the invention, the V block
having a V value of 8 and an angle of 30°;
Figure 12 depicts a lead-in curve of a V block according to the invention, the V block
having a V value of 6 and an angle of 30°;
Figure 13 depicts a lead-in curve of a V block according to the invention, the V block
having a V value of 16 and an angle of 86°.
[0049] In Figures 7, 8, 9 and 10, the same variables (reaction force, contact pressure,
slip speed/rolling speed, and wear) are presented for a V block according to the invention
as a function of the bending angle (j) as were presented on Figures 2, 3, 4 and 5
for a known V block.
[0050] A comparison of the respective Figures clearly shows that both the contact pressure
(σj) and the wear (Wej) of the V block are considerably reduced when a V block according
to the invention is used.
[0051] The drawbacks indicated of the known V blocks have thus been overcome. The contact
pressure (σj) remains - if the V value of the V block is chosen correctly - below
the value at which imprinting of the plate or sheet is caused. The slip speed is smaller,
compared to the rolling speed (in particular at bending angles at which the contact
pressure is the largest) so that (partly owing to the limited contact pressure) the
marks in the plate or sheet are prevented, and the wear of the V block becomes much
smaller.
[0052] Figures 11, 12, 13 depict the course of the lead-in curve, as it is preferentially
implemented in practice, by approximating the optimal curve by composing it from a
large number of successive sections having a constant radius of curvature (r), according
to the equations from Claim 7.
[0053] In the Tables below, with the aid of the respective examples of Figures 11, 12 and
13, the values of r, x
c, y
c calculated according to these equations are given for the successive sections of
the curve situated between the points having coordinates (x, y), which are calculated
according to the equations for the optimal curve from Claims 5 or 6.
| 1. For V=8 with an angle of 30° (see Figure 11) |
| x |
y |
r |
xc |
yc |
| 0.000 |
0.000 |
|
|
|
| 1.841 |
0.000 |
1.581 |
1.841 |
-1.581 |
| 1.979 |
-0.006 |
1.756 |
1.826 |
-1.755 |
| 2.131 |
-0.026 |
1.949 |
1.792 |
-1.946 |
| 2.297 |
-0.063 |
2.165 |
1.736 |
-2.154 |
| 2.477 |
-0.120 |
2.403 |
1.655 |
-2.378 |
| 2.670 |
-0.201 |
2.668 |
1.543 |
-2.619 |
| 2.877 |
-0.308 |
2.963 |
1.395 |
-2.874 |
| 3.095 |
-0.447 |
3.289 |
1.208 |
-3.142 |
| 3.323 |
-0.622 |
3.652 |
0.975 |
-3.420 |
| 3.557 |
-0.838 |
4.055 |
0.690 |
-3.705 |
| 3.796 |
-1.099 |
4.502 |
0.348 |
-3.993 |
| 4.035 |
-1.411 |
4.998 |
-0.059 |
-4.278 |
| 4.270 |
-1.779 |
5.548 |
-0.535 |
-4.554 |
| 4.493 |
-2.210 |
6.158 |
-1.088 |
-4.812 |
| 4.699 |
-2.707 |
6.834 |
-1.723 |
-5.044 |
| 4.878 |
-3.277 |
<--- end of profile |
|
| 2. For V=6 with an angle of 30° (see Figure 12) |
| x |
y |
r |
xc |
yc |
| 0.000 |
0.000 |
|
|
|
| 3.705 |
0.000 |
0.949 |
3.705 |
-0.949 |
| 3.787 |
-0.004 |
1.053 |
3.695 |
-1.053 |
| 3.878 |
-0.016 |
1.170 |
3.675 |
-1.168 |
| 3.978 |
-0.038 |
1.299 |
3.642 |
-1.292 |
| 4.086 |
-0.072 |
1.442 |
3.593 |
-1.427 |
| 4.202 |
-0.120 |
1.601 |
3.526 |
-1.571 |
| 4.326 |
-0.185 |
1.778 |
3.437 |
-1.724 |
| 4.457 |
-0.268 |
1.974 |
3.325 |
-1.885 |
| 4.594 |
-0.373 |
2.191 |
3.185 |
-2.052 |
| 4.734 |
-0.503 |
2.433 |
3.014 |
-2.223 |
| 4.878 |
-0.659 |
2.701 |
2.809 |
-2.396 |
| 5.021 |
-0.847 |
2.999 |
2.565 |
-2.567 |
| 5.162 |
-1.068 |
3.329 |
2.279 |
-2.732 |
| 5.296 |
-1.326 |
3.695 |
1.947 |
-2.887 |
| 5.419 |
-1.624 |
4.101 |
1.566 |
-3.027 |
| 5.527 |
-1.966 |
<--- end of profile |
|
| 3. For V=16 with an angle of 30° (see Figure 13) |
| x |
y |
r |
xc |
yc |
| 0.000 |
0.000 |
|
|
|
| 2.998 |
0.000 |
2.480 |
2.998 |
-2.480 |
| 3.134 |
-0.004 |
2.649 |
2.989 |
-2.648 |
| 3.278 |
-0.016 |
2.828 |
2.970 |
-2.827 |
| 3.432 |
-0.037 |
3.020 |
2.938 |
-3.016 |
| 3.594 |
-0.068 |
3.225 |
2.894 |
-3.216 |
| 3.765 |
-0.111 |
3.444 |
2.835 |
-3.427 |
| 3.945 |
-0.167 |
3.677 |
2.760 |
-3.648 |
| 4.133 |
-0.237 |
3.926 |
2.666 |
-3.879 |
| 4.330 |
-0.323 |
4.193 |
2.554 |
-4.120 |
| 4.535 |
-0.426 |
4.477 |
2.419 |
-4.371 |
| 4.747 |
-0.547 |
4.780 |
2.261 |
-4.630 |
| 4.967 |
-0.689 |
5.104 |
2.078 |
-4.898 |
| 5.193 |
-0.854 |
5.451 |
1.867 |
-5.172 |
| 5.424 |
-1.042 |
5.820 |
1.626 |
-5.452 |
| 5.659 |
-1.256 |
6.215 |
1.352 |
-5.737 |
| 5.897 |
-1.499 |
<--- end of profile |
|
1. V block (1) for bending plates or sheets (3), consisting of a solid piece having at
least one flat side, which via roundings merges into the flanks of an elongated recess
having a V- shaped profile which is provided in said flat side, while the profile
of the recess and of said roundings - called lead-in curves - is identical over their
entire length, characterized in that the roundings in profile have a lead-in curve
(2) whose radius of curvature (ρ) adopts at least two different values, and in that
at at least one point on the lead-in curve (2) the radius of curvature (ρ) is greater
than the radius of curvature (ρi) of the start of the lead-in curve - where it merges
into the flat side (8) of the V block (1).
2. V block (1) according to Claim 1, characterized in that the different values of the
radius of curvature (ρ) increase from the flat side (8) towards the flank (6) of the
recess (7).
3. V block (1), according to Claim 1 or 2, characterized in that the ratio of the radius
of curvature (pe) of the end of the lead-in curve - where it merges into a flank of
the recess - with respect to the radius of curvature (ρi) of the start of the lead-in
curve - where it merges into the flat side of the V block - for a V block having an
angle β is within the limits defined by the following formulae:
Lower limit:

Upper limit:
4. V block (1) according to Claim 3, characterized in that the ratio

is equal to
5. V block (1) according to one or more of the preceding claims, characterized in that
the profile of a lead-in curve (2) has the coordinates (x, y), defined by the following
equations, in a rectangular set of x-y axes having its origin in the starting point
of the curve (where it merges into the flat side (8) of the V block (1)) and having
a horizontal X axis in the extension of that flat side (8), and directed towards the
other lead-in curve (2), and having a vertical, upwards-directed Y axis


with 0 ≦ φ ≦ 90°-β/2 (β > 0°)
in which:
- m is a constant value from 1.1 to 1.5 inclusive,
- φ is the angle, varying from 0 to 90°-β/2, which is formed between the Y axis and
the straight line perpendicular to the rounding
- α = tan⁻¹ (m)
- β is the angle of the V block
- ρi is the radius of curvature of the start of the curve.
6. V block (1) according to Claim 5, characterized in that m = 1.2.
7. V block (1) according to Claim 5 or 6, characterized in that the lead-in curve having
coordinates (x, y) is approximated by composing it from a number of portions having
a constant radius of curvature, in that the coordinates of start and end point of
each portion are defined according to the equations according to Claim 5 or 6, in
that the value of the radius of curvature (r) is defined according to the following
equation:

in which:
xi+1: is the x coordinate of the end point of a particular portion of the lead-in curve
xi: is the x coordinate of the starting point of that portion
φi+1: is the value of the angle φ for the end point of that portion of the lead-in curve
φi: is the value of the angle φ for the starting point of that portion of the lead-in
curve
and in that the coordinates (x
c, y
c) of the centre of curvature of each portion are defined according to the following
equations:


in which (x
i, y
i) are the coordinates of the starting point of the portion having the constant radius
of curvature.