This is a continuation of International Application No. PCT/JP2013/001847 filed on Mar. 18, 2013, which claims priority to Japanese Patent Application No. 2012-061594 filed on Mar. 19, 2012. The entire disclosures of these applications are incorporated by reference herein.
The present disclosure relates to V-belts for high load transmission, and more particularly to those preferably used for belt-type continuously variable transmissions.
This type of V-belts for high load transmission have been well known, and, for example, have been wound between variable speed pulleys of belt-type continuously variable transmissions. Each V-belt for high load transmission includes tension bands, each having numbers of, for example, upper and lower recessed grooves arranged at regular intervals in the upper surface facing the back of the belt and the lower surface facing the bottom of the belt in the belt length direction to vertically correspond to each other. Each V-belt also includes numbers of blocks, each including fit portions in which the tension bands are press-fitted, for example, an upper projecting tooth formed in the upper surfaces of the fit portions and meshing with the upper grooves of the tension bands, and, for example, a lower projecting tooth formed in the lower surfaces of the fit portions and meshing with the lower grooves of the tension bands. The V-belts are also called block belts.
Each tension band includes a cord reducing expansion of the belt and transmitting power, a shape-retaining rubber layer, a canvas reducing friction with the blocks, etc.
The blocks are made of resin such as phenolic resin. Each block includes an upper beam at the back of the belt, and a lower beam at the bottom of the belt. The fit portions of the tension bands are formed between the upper and lower beams.
The tension bands are press-fitted in the fit portions of the blocks, thereby engaging the blocks with the tension bands, with the projecting teeth and the recessed grooves meshing at regular intervals in the belt length direction. The teeth of the blocks and the grooves of the tension bands are integrated by the meshing to transmit power.
Such a V-belt for high load transmission provides a protruding margin, which is the protrusion of the outer end surface of each tension band in the width direction beyond the contact surfaces of the blocks with a pulley (see, e.g., for example, Japanese Patent No. 4256498). Then, when the belt is wound around the pulley, the protruding margin of the tension band is pressed inside in the belt width direction such that the tension band vertically expands in the fit portions. As a result, the blocks are firmly held by the tension band. In such a V-belt for high load transmission, the side surfaces of the blocks and the tension band in the belt width direction abut on the groove surface of the pulley.
The present inventor found the following phenomenon in the above-described V-belt for high load transmission. When the belt is wound around a variable speed pulley to run, the thrust applied from the groove surface of the pulley to the contact surface of the belt with the pulley generates the belt tension. As the running time passes from the initial running stage of the belt, the thrust-tension conversion ratio changes. If the thrust-tension conversion ratio changes, desired belt tension may not be obtained.
In order to secure desired belt tension in a long running period of the belt, a drive unit opening and closing the variable speed pulley is suggested to have excessive thrust including a safety factor to some extent. This increases the load applied to the belt to deteriorate the durability and increase noise.
The present disclosure aims to provide a V-belt for high load transmission, which reduces a temporal change in the belt tension according to a change in the thrust-tension conversion ratio from the initial running stage of the belt, not requiring the excessive thrust.
The present inventor studied the phenomenon of the change in the thrust-tension conversion ratio, and found that the change is generated by the following two mechanisms.
Specifically, in the V-belts for high load transmission, the resin which is the component of the blocks has a higher coefficient of thermal expansion than the rubber which is the component of each tension band. When the belt is wound around the variable speed pulley to run, due to the thermal expansion of the tension band, the lower beams of the blocks are bound to the tension band, and are not pushed up. However, the upper beams are pushed up to increase the distance between the upper and lower beams. The side surfaces of the lower beams mainly abut on the groove surface of the pulley. This reduces the thrust-tension conversion ratio to reduce the belt tension.
After that, when the tension band is fatigued with the running of the belt, the expansion of the upper beams decreases, and the side surfaces of the upper beams also abut on the groove surface of the pulley. As a result, the thrust-tension conversion ratio increases to increase the belt tension. As such, the thrust-tension conversion ratio changes as the running time passes from the initial running stage of the belt.
The other mechanism is caused by the dependency of the thrust-tension conversion ratio on the coefficient of friction of the belt. Specifically, when the belt is wound around the variable speed pulley to run, the thermal expansion of the tension band increases the ratio of the tension band to the contact surface of the belt with the pulley. Since the tension band (i.e., rubber) has a higher coefficient of friction than the blocks (i.e., resin), the coefficient of friction of the belt as a whole increases with the increasing the ratio of the tension band. As a result, the thrust-tension conversion ratio increases to increase the belt tension.
After that, when the tension band is worn in accordance with the running of the belt, the ratio of the tension band to the contact surface of the belt with the pulley decreases to decrease the coefficient of friction of the belt as a whole. As a result, the thrust-tension conversion ratio decreases to decrease the belt tension.
These two mechanisms change the thrust-tension conversion ratio as the running time passes from the initial running stage of the belt. The present inventor focused on reducing the influence of the thermal expansion of the tension band, which is common between these two mechanisms, and completed the present disclosure.
Specifically, the present disclosure provides a V-belt for high load transmission including tension bands, each including a cord buried inside a shape-retaining rubber layer, and numbers of upper and lower grooves arranged in a belt length direction to vertically correspond to each other, the upper grooves being formed in an upper surface facing a back of the belt, and the lower grooves being formed in a lower surface facing a bottom of the belt; and numbers of blocks, each including fit portions in which the tension bands are press-fitted, an upper tooth formed in upper surfaces of the fit portions and meshing with the upper grooves of the tension bands, and a lower tooth formed in lower surfaces of the fit portions and meshing with the lower grooves of the tension bands. The tension bands are fitted in the fit portions of the blocks, thereby engaging and fixing the blocks with and to the tension bands. Meshing of the teeth of the blocks with the grooves of the tension bands transmits power.
Side surfaces of each tension band and the blocks in a belt width direction form sliding surfaces abutting on a groove surface of a pulley.
An area S1 of the sliding surface of the tension band and an area S2 of the sliding surface of each of the blocks satisfy a relationship of S1/S2≦0.2 (i.e., the area of the side surface of the tension band is 20% or smaller of the area of the side surface of each block).
A ratio S1/S2 of the area S1 of the sliding surface of the tension band to the area S2 of the sliding surface of each of the blocks may range from 0.13 to 0.2.
The area S1 of the sliding surface of the tension band may range from 4.3 to 8.5 mm2. The area S2 of the sliding surface of each of the blocks may range from 33 to 43 mm2.
This structure provides the following effects and advantages. If the ratio S1/S2 of the area S1 of the sliding surface of the tension band to the area S2 of the sliding surface of each of the blocks is higher than 0.2, the ratio of the tension band to the contact surface of the belt with the pulley is high. Then, the tension band thermally expands to push up the upper beams of the blocks, and increase the coefficient of friction of the belt. However, in the present disclosure, the ratio S1/S2 of the area S1 of the sliding surface of the tension band to the area S2 of the sliding surface of each of the blocks is 0.2 or smaller. That is, the ratio of the tension band to the contact surface of the belt with the pulley is sufficiently low. Thus, the upper beams of the blocks are not pushed up by the thermal expansion of the tension band, and an increase in the coefficient of friction of the belt is reduced. This reduces the change in the thrust-tension conversion ratio and the change in the belt tension according thereto with the running time of the belt. As a result, the thrust of the drive unit decreases to reduce the initial heat built-up of the belt, and to improve the efficiency and the durability of the belt.
A belt pitch width a being a belt width at a position of the cord of each tension band, and a meshing thickness b of the tension band between lower ends of the upper grooves and upper ends of the lower grooves satisfy a relationship of b/a≦0.08.
This structure reduces bending loss of the belt. This further reduces the change in the thrust-tension conversion ratio with the running time of the belt.
Furthermore, the belt pitch width a and the meshing thickness b of the tension band may satisfy a relationship of b/a≦0.05.
This structure significantly reduces the bending loss of the belt, and more effectively reduces the change in the thrust-tension conversion ratio with the running time of the belt.
The V-belt for high load transmission may be wound around a variable speed pulley of a belt-type continuously variable transmission.
This structure provides a V-belt for high load transmission efficiently exhibiting the advantages of the present disclosure.
According to the present disclosure, the area S1 of the sliding surface of the tension band of the V-belt for high load transmission and the area S2 of the sliding surface of each of the blocks satisfy the relationship of S1/S2≦0.2. This reduces the temporal change in the belt tension from the initial running stage of the belt according to a change in the thrust-tension conversion ratio. As a result, the thrust of the drive unit decreases to reduce the initial heat built-up of the belt, and to improve the efficiency and the durability of the belt.
An embodiment of the present disclosure will be described hereinafter in detail with reference to the drawings. The following description of the preferred embodiment is intrinsically a mere example, and is not intended to limit the present disclosure, equivalents, and application.
As also shown in
The hard rubber of the shape-retaining rubber layer 1a is formed by reinforcing H-NBR rubber reinforced by, for example, zinc methacrylate, using short fibers such as aramid fibers and nylon fibers. Thus, the hard rubber highly heat resistive and less subject to permanent deformation is used. The hard rubber needs to have a hardness of 75° or higher when measured with a JIS-C hardness meter.
Upper and lower canvas layers 6 and 7 are formed on the upper and lower surfaces of each tension band 1 by integrally adhering canvases, which have been subjected to glue rubber processing.
On the other hand, as shown in
The blocks 10 are fixed to the tension bands 1 and 1 by press-fitting the tension bands 1 and 1 in the fit portions 11 and 11. Specifically, as shown in
A meshing thickness b of each tension band is slightly greater than a meshing thickness d of each block (b>d). The meshing thickness b is the thickness of each tension band 1 made of the hard rubber between the upper and lower recesses 2 and 3, that is, as shown in
As shown in
When this V-belt B for high load transmission is wound around the pulley to run, the upper and lower projections (i.e., the teeth) 15 and 16 of the blocks 10 mesh with the upper and lower recesses (i.e., the grooves) 2 and 3 of the tension bands 1, thereby transmitting power.
In this V-belt B for high load transmission, in order to reduce the change in the thrust-tension conversion ratio with the running time of the belt, as shown in
S1/S2≦0.2 (1)
That is, the area S1 of the sliding surface 1c of each tension band is 20% or smaller of the area S2 of the sliding surface 12 of each block. Specifically, the ratio S1/S2 preferably ranges from 0.13 to 0.2. For example, the area S1 of the sliding surface 1c of each tension band preferably ranges from 4.3 to 8.5 mm2, and the area S2 of the sliding surface 12 of each block preferably ranges from 33 to 43 mm2.
As shown in
b/a≦0.08 (2)
That is, the meshing thickness b of each tension band is 8% or smaller of the belt pitch width a. A more preferable relationship is as follows.
b/a≦0.05 (3)
(That is, the meshing thickness b of each tension band is 5% or smaller of the belt pitch width a.)
The belt pitch width a is related to the holding area of the tension band 1 holding the blocks 10. Thus, in addition to reducing the meshing thickness b of each tension band, the meshing thickness b of each tension band and the belt pitch width a need to satisfy the above expression (1) or (2).
This V-belt B for high load transmission has the above-described structure. The effects and advantages of this V-belt B for high load transmission will be described next. In this V-belt B for high load transmission, the area S1 of the sliding surface of the each tension band and the area S2 of the sliding surface of each block satisfy the relationship of S1/S2≦0.2. That is, the ratio of the tension band 1 to the contact surface of the belt B with the pulley is sufficiently small. This reduces push-up of the upper beams 10a of the blocks 10 caused by the thermal expansion of the tension band 1, and an increase in the coefficient of friction of the belt, when the belt B is wound around a variable speed pulley of, for example, a continuously variable transmission to run. Thus, the change in the thrust-tension conversion ratio, and the change in the belt tension according thereto are reduced, even after the running time of the belt B has passed. This reduces the thrust (i.e., the thrust pushing a movable sheave of the variable speed pulley in the axis direction) of a drive unit, which opens and closes the variable speed pulley of the transmission to change the gear ratio. As a result, the initial heat built-up of the belt B decreases, and the efficiency and the durability of the belt B improve.
Since the belt pitch width a and the meshing thickness b of each tension band satisfy the relationship of b/a≦0.08, the meshing thickness b of each tension band is sufficiently small relative to the belt pitch width a, thereby reducing bending loss of the belt B. This further reduces the change in the thrust-tension conversion ratio with the running time of the belt B. Where the belt pitch width a and the meshing thickness b of each tension band satisfy the relationship of b/a≦0.05, the change in the thrust-tension conversion ratio with the running time of the belt B decreases more effectively.
In this embodiment, the reinforcing member 18 is inserted into each block. In the present disclosure, however, the entire blocks may be made of resin without using the reinforcing member 18. This structure provides similar effects and advantages.
The V-belt B for high load transmission according to this embodiment is not only wound around the variable speed pulley of the belt-type continuously variable transmission, but may be used for belt-type transmissions including a constant speed pulley (i.e., a V pulley).
Next, specifically conducted examples will be described. V-belts for high load transmission having the structure of the above-described embodiment are fabricated as first to sixth examples and first to third comparative examples. The belt angle α of each belt (i.e., the angle between the sliding sections of the side surfaces of each block) is 26°. The belt pitch width a is 25 mm. The pitch P of the blocks in the belt length direction is 3 mm. The thickness of each block (i.e., the thickness in the belt length direction) is 2.95 mm. Each protruding margin Δe ranges from 0.05 to 0.15 mm. The belt length is 612 mm.
Each used block is formed by inserting and molding a reinforcing member made of a high-strength light aluminum alloy with a thickness 2 mm into phenolic resin. Blocks, which are entirely made of resin without using the reinforcing member made of the aluminum alloy, provide similar advantages.
The belts according to the first to sixth examples and the first to third comparative examples have different areas S1 of the sliding surfaces 1c of the tension bands, different areas S2 of the sliding surfaces 12 of the blocks, and different meshing thicknesses b of the tension bands (see
The area S1 of the sliding surface 1c of each tension band is 6.7 mm2. The area S2 of the sliding surface 12 of each block is 33 mm2. The meshing thickness b of each tension band is 1.6 mm. Therefore, the S1/S2 is 0.20 (i.e., 20%), and b/a is 0.064 (i.e., 6.4%).
The area S1 of the sliding surface 1c of each tension band is 6.4 mm2. The area S2 of the sliding surface 12 of each block is 33 mm2. The meshing thickness b of each tension band is 1.5 mm. Therefore, S1/S2 is 0.19 (i.e., 19%), and b/a is 0.060 (i.e., 6.0%).
The area S1 of the sliding surface 1c of each tension band is 5.5 mm2. The area S2 of the sliding surface 12 of each block is 33 mm2. The meshing thickness b of each tension band is 1.2 mm. Therefore, S1/S2 is 0.17 (i.e., 17%), and b/a is 0.048 (i.e., 4.8%).
The area S1 of the sliding surface 1c of each tension band is 4.9 mm2. The area S2 of the sliding surface 12 of each block is 33 mm2. The meshing thickness b of each tension band is 1 mm. Therefore, S1/S2 is 0.15 (i.e., 15%), and b/a is 0.040 (i.e., 4.0%).
The area S1 of the sliding surface 1c of each tension band is 4.3 mm2. The area S2 of the sliding surface 12 of each block is 33 mm2. The meshing thickness b of each tension band is 0.8 mm. Therefore, S1/S2 is 0.13 (i.e., 13%), and b/a is 0.032 (i.e., 3.2%).
The area S1 of the sliding surface 1c of each tension band is 8.5 mm2. The area S2 of the sliding surface 12 of each block is 43 mm2. The meshing thickness b of each tension band is 2.2 mm. Therefore, S1/S2 is 0.20 (i.e., 20%), and b/a is 0.088 (i.e., 8.8%).
The area S1 of the sliding surface 1c of each tension band is 8.5 mm2. The area S2 of the sliding surface 12 of each block is 33 mm2. The meshing thickness b of each tension band is 2.2 mm. Therefore, S1/S2 is 0.26 (i.e., 26%), and b/a is 0.088 (i.e., 8.8%).
The area S1 of the sliding surface 1c of each tension band is 11.4 mm2. The area S2 of the sliding surface 12 of each block is 33 mm2. The meshing thickness b of each tension band is 3 mm. Therefore, S1/S2 is 0.35 (i.e., 35%), and b/a is 0.12 (i.e., 12%).
The area S1 of the sliding surface 1c of each tension band is 13.9 mm2. The area S2 of the sliding surface 12 of each block is 33 mm2. The meshing thickness b of each tension band is 4 mm. Therefore, S1/S2 is 0.42 (i.e., 42%), and b/a is 0.16 (i.e., 16%).
The temporal change in the belt tension, the high-speed durability, the initial heat built-up, the change in the fastening margin, and belt efficiency are evaluated in each of the above-described examples and comparative examples.
The temporal change in the belt tension was measured in each of the examples and the comparative examples using equipment measuring and testing the belt tension (i.e., inter-shaft power) shown in
The high-speed, high-load durability and the heat resistance were measured in each of the examples and the comparative examples using equipment for testing high-speed durability shown in
At the test of the high-speed, high-load durability and the heat resistance, the heating temperature of each belt B at the initial running stage (2hours after the start of running) was measured.
At the test of the high-speed, high-load durability and the heat resistance, the change in the fastening margin after 250 hours has passed after the start of running was measured. The fastening margin was obtained by subtracting the meshing thickness d of each block from the thickness b of each tension band.
The belt efficiency was measured in the examples and the comparative examples using test equipment shown in
efficiency η (%)={(speed of driven pulley×torque of driven pulley)/(speed of drive pulley×torque of drive pulley)}×100
In
The above-described results show that, in the first to sixth examples, in which the area S1 of the sliding surface 1c of each tension band is 20% or smaller of the area S2 of the sliding surface 12 of each block, the variation range of the belt tension is 200 N or lower. That is, the temporal change is small. On the other hand, in the first to third comparative examples, the area S1 of the sliding surface 1c of each tension band is greater than 20% of the area S2 of the sliding surface 12 of each block. That is, the variation range of the belt tension is as wide as 900 N or more. From the foregoing, it is found that a change in the thrust-tension conversion ratio with the running time of the belt is reduced by setting the area S1 of the sliding surface 1c of each tension band to be 20% or smaller of the area S2 of the sliding surface 12 of each block.
In the first to sixth examples, the area S1 of the sliding surface 1c of each tension band is 20% or smaller of the area S2 of the sliding surface 12 of each block. These examples clearly show that the high-speed durability, the initial heat built-up, the change in the fastening margin, and the belt efficiency dramatically improve. These examples are significantly distinguishable from the first to third comparative examples.
Furthermore, in the first to fifth examples in which the meshing thickness b of each tension band is 8% or smaller of the belt pitch width a, the variation range of the belt tension is 100 N or narrower. In particular, in the third to fifth examples in which the meshing thickness b of each tension band is 5% or smaller of the belt pitch width a, the variation range of the belt tension is 0 N. That is, there is no temporal change. From the foregoing, it is found that the change in the thrust-tension conversion ratio with the running time of the belt is reduced by setting the meshing thickness b of each tension band to be 8% or smaller of the belt pitch width a.
As compared to conventional art, the present disclosure reduces the temporal change in the tension in running the belt, and provides dramatically high performance such as heat built-up, running durability, and belt efficiency. Therefore, the present disclosure is significantly useful and is highly industrially applicable in utilizing for belts of continuously variable transmissions such as vehicles and two-wheel scooters.
Number | Date | Country | Kind |
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2012-061594 | Mar 2012 | JP | national |
Number | Date | Country | |
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Parent | PCT/JP2013/001847 | Mar 2013 | US |
Child | 14491078 | US |