The present invention relates to a dynamic damper mounted on a rotational shaft such as a drive shaft of an automobile or the like, for dampening hazardous vibrations developed on the rotational shaft.
Heretofore, there is known a dynamic damper mounted on a rotational shaft such as a drive shaft or a propeller shaft of an automobile or the like, for damping hazardous vibrations which should not be caused, such as flexural vibrations, torsional vibrations, etc. that are developed due to an unbalanced rotational behavior caused when the rotational shaft rotates.
The dynamic damper has a function to absorb the vibrational energy of the rotational shaft by converting the vibrational energy into vibrational energy of the dynamic damper by way of resonance, with the natural frequency of the dynamic damper being equal to the dominant frequency of excited hazardous vibrations of the rotational shaft.
One dynamic damper of the above type, which is disclosed in Japanese Laid-Open Patent Publication No. 11-101306, for example, comprises a tubular member of rubber having a boss with a rotational shaft press-fitted therein and a joint support integrally formed with an outer surface of the boss, a ring-shaped mass member disposed radially outwardly of the boss and elastically joined to and supported on the boss by the joint support, and a ring-shaped securing fitting for securing the boss to the rotational shaft. The disclosed dynamic damper allows the rotational shaft to be fitted and mounted easily therein and makes the securing member resistant to corrosion.
Japanese Laid-Open Patent Publication No. 2003-254387 discloses a dynamic damper having two different first and second vibroisolating members which are mounted together on a drive shaft. The dynamic damper can dampen vibrations at two different natural frequencies of the drive shaft to be controlled, by independently adjusting the properties and structures of rubber elastomers of the first and second vibroisolating members.
When the dynamic dampers disclosed in Japanese Laid-Open Patent Publication No. 11-101306 and Japanese Laid-Open Patent Publication No. 2003-254387 are actually manufactured, since they are complexly shaped, the manufacturing operation and the manufacturing process are complex, and they are costly to manufacture.
Specifically, if the dynamic dampers are manufactured by pouring a rubber material into a mold, then since the dynamic dampers disclosed in Japanese Laid-Open Patent Publication No. 11-101306 and Japanese Laid-Open Patent Publication No. 2003-254387 are complex in shape and structure, the mold has a complex cavity structure and is of a high cost, which is reflected in the cost of the products.
As vehicles are becoming more compact and more space saving in recent years, their engine compartments are also becoming smaller in volume. Accordingly, there are demands for smaller dynamic dampers. Different vehicle types have different dimensions and shapes as to engine compartment spaces and engine components. As the layout of mechanisms and devices mounted on automobile bodies, i.e., the vehicle layout, has a low level of freedom, it is necessary that the dimensions and shapes of dynamic dampers be individually set out of interference with surrounding mechanisms and devices. Consequently, dynamic dampers and molds for dynamic dampers need to be prepared in a vast range of types, resulting in high equipment investments.
It is a general object of the present invention to provide a dynamic damper which is simple and small in shape and structure, so that a cavity structure of a mold for forming the dynamic damper is simplified to reduce the cost incurred to manufacture the dynamic damper.
According to the present invention, wall surfaces between a plurality of adjacent mass members are provided by flat surfaces that confront each other. Therefore, they provide a simple shape for allowing a mold to be easily removed when the mold is opened, and hence the dynamic damper can easily be manufactured.
According to the present invention, furthermore, by setting a spaced distance A and the width B of the mass members to satisfy the positional relationship A≦(B/3) between joint supports and the mass members, the lateral moment of the mass members along the axial direction of a rotational shaft can be suppressed, and the mass members can be set to a desired resonant frequency. Consequently, the vibrations of the rotational shaft are reliably attenuated by tensile/compressive deformation or shearing deformation (resonance).
According to the present invention, when the rotational shaft rotates, the joint supports may be subjected to tensile/compressive deformation in a diametrical direction of the rotational shaft, or may be subjected to shearing deformation in a circumferential direction of the rotational shaft. The joint supports may be simultaneously subjected to tensile/compressive deformation and shearing deformation.
The tensile/compressive deformation refers to the deformation of the joint supports as they are extended or compressed in the diametrical direction of the rotational shaft. The shearing deformation refers to the deformation of the joint supports as they are pulled in the circumferential direction of the rotational shaft, i.e., a direction opposite to the direction in which the rotational shaft rotates.
The drive force transmitting mechanism 10 comprises a drive shaft 12, and a Barfield constant velocity universal joint 14 and a tripod constant velocity universal joint 16 which are joined to the respective ends of the drive shaft 12. Joint boots 18, 20 made of rubber or resin are mounted respectively on the Barfield constant velocity universal joint 14 and the tripod constant velocity universal joint 16. A dynamic damper 22 is mounted substantially centrally on the drive shaft 12 by a band, not shown.
As shown in
The main body 24 has a through hole 30 defined therein, and the drive shaft 12 extends through the through hole 30. The non-illustrated band is wound in an annular recess 32 defined in a circumferential side wall of the main body 24. When the band is tightened, the dynamic damper 22 is positioned and secured in position on the drive shaft 12.
The joint supports 28a, 28b project from the main body 24 diametrically outwardly of the drive shaft 12, and are flexible to support the mass members 26a, 26b elastically.
Specifically, as shown in
As shown in
Since the wall surfaces between the mass members 26a, 26b are provided by the flat surfaces 31, 31 that face each other, the dynamic damper can easily be removed from a mold when the mold is opened (described later), and hence can simply be manufactured.
The annular mass members 26a, 26b which extend around the circumferential side wall of the drive shaft 12 have respective annular spaces 34a, 34b of rectangular cross section defined therein. Weights 36a, 36b are housed respectively in the spaces 34a, 34b. When the drive shaft 12 is vibrated, the weights 36a, 36b are displaced in unison with the mass members 26a, 26b.
The weights 36a, 36b each comprise a sintered body produced when a powder of tungsten alloy mixed with a metal binder is sintered. However, the weights 36a, 36b may each comprise a molded body produced by a metal injection molding (MIM) process or a powder injection molding (PIM) process, rather than a sintered body. The weights 36a, 36b thus constructed have a specific gravity which generally exceeds 14, e.g., a high specific gravity of 17 or more, and hence have a very large weight.
Preferred examples of tungsten alloy are W-1.8Ni-1.2Cu (a specific gravity of 18.5, the numerals prior to the elements represent weight %, the same being true with the examples below), W-3.0Ni-2.0Cu (a specific gravity of 17.8), W-5.0Ni-2.0Fe ((a specific gravity of 17.4), and W-3.5Ni-1.5Fe ((a specific gravity of 17.6), etc. The specific gravity of the weights 36a, 36b made of tungsten alloy is more than twice weights made of an iron material. If the weights 36a, 36b have the same mass as weights made of an iron material, then the weights 36a, 36b have a volume which is about ⅓ to ½ of those weights.
In other words, if the weights 36a, 36b are made of tungsten alloy, then their size is much smaller than the conventional weights of an iron material.
The positional relationship between the mass member 26a (26b) and the joint support 28a (28b) will be described below.
As shown in
The above dimensional relationship includes the instance wherein the central point C (D/2) of the joint support 28a (28b) along the axis of the drive shaft 12 is aligned with the center G of gravity of the weight 36a (36b), so that the spaced distance A between the central point C of the joint support 28a (28b) and the center G of gravity of the weight 36a (36b) is 0.
By setting the spaced distance A and the width B of the mass member 26a (26b) to satisfy the relationship A≦B/3, a lateral moment of the mass members 26a, 26b along the axis of the drive shaft 12 can be suppressed, and the mass members 26a, 26b can be set to a desired resonant frequency. The above relationship is applicable to not only the two mass members 26a, 26b, but also to all two or more mass members.
Stated otherwise, if the relationship A≦B/3 is not satisfied, then a lateral moment of the mass member 26a (26b) increases, making it difficult to set the mass member 26a (26b) to a desired resonant frequency, and the mass member 26a (26b) may possibly have a portion brought into contact with the drive shaft 12 or the main body 24, adversely affecting them.
As shown in
Since the flat surfaces 31, 31 are provided between the two mass members 26a, 26b, the mold 64 can easily be opened by displacing the left and right molds 63a, 63b in horizontal directions (indicated by the arrows in
The dynamic damper 22 according to the present embodiment is basically constructed as described above. Operation and advantages of the dynamic damper 22 will be described below.
First, the drive shaft 12 is inserted to a given position through the through hole 30 defined in the main body 24 of the dynamic damper 22. Thereafter, the non-illustrated band is wound and tightened in the annular recess 32 of the main body 24. The dynamic damper 22 is now positioned and fixed in the predetermined position on the drive shaft 12.
According to the present embodiment, since the wall surfaces between the two mass members 26a, 26b are a pair of the flat surfaces 31, 31, they provide a simple shape for allowing the mold 64 (the left and right molds 63a, 63b) to be easily removed when the mold 64 is opened, as shown in
In the drive force transmitting mechanism 10 mounted on a vehicle, the dynamic damper 22 is mounted on the drive shaft 12 as described above. According to the present embodiment, the weights 36a, 36b and hence the mass members 26a, 26b are very small in volume. Therefore, as the dynamic damper 22 is prevented from interfering with surrounding mechanisms and devices, those mechanisms and devices can be laid out with increased freedom in the vehicle. Stated otherwise, a wider choice of vehicle layouts is available.
Inasmuch as the dynamic damper 22 can be installed in various vehicle layouts, the range of vehicles that can be selected for the installation of the dynamic damper 22 is greatly increased. Stated otherwise, it is unnecessary to change the dimensions or the shape of the dynamic damper 22 depending on the types of vehicles. Thus, the trouble of having to design many types of dynamic dampers is eliminated, and equipment investments are lowered because there is no need for the preparation of many types of molds.
According to the present embodiment, since the weights 36a, 36b and hence the mass members 26a, 26b are reduced in size, a plurality of mass members 26a, 26b can be provided (see
When the drive shaft 12 is vibrated for some reasons, the mass members 26a, 26b which accommodate the respective weights 36a, 36b are subjected to at least one of tensile/compressive deformation and shearing deformation.
Specifically, when the drive shaft 12 is undesirably vibrated, the vibrations are transmitted from the main body 24 through the joint supports 28a, 28b to the mass members 26a, 26b. At this time, the mass members 26a, 26b which accommodate the respective weights 36a, 36b and have their resonant frequency matching the frequency of the unwanted vibrations are extended and contracted from the joint supports 28a, 28b along the diametrical direction of the drive shaft 12, i.e., are subjected to tensile/compressive deformation.
The joint supports 28a, 28b may be deformed so as to be pulled along a circumferential direction of the drive shaft 12, i.e., a direction opposite to the direction in which the drive shaft 12 rotates, or in other words may be subjected to shearing deformation. Of course, the joint supports 28a, 28b may be simultaneously subjected to tensile/compressive deformation and shearing deformation.
Upon the tensile/compressive deformation or the shearing deformation, the mass members 26a, 26b (the weights 36a, 36b) resonate. Since the mass members 26a, 26b are essentially identical in shape to each other, they have essentially the same resonant frequency, and hence absorb the vibrational energy developed in the drive shaft 12 and appropriately suppress vibrations.
Specifically, the vibrations of the drive shaft 12 are attenuated when the mass members 26a, 26b (the weights 36a, 36b) elastically supported by the flexible joint supports 28a, 28b resonate.
By setting the spaced distance A and the width B of the mass members 26a, 26b to satisfy the positional relationship A≦(B/3) between the joint supports 28a, 28b and the mass members 26a, 26b, the lateral moment of the mass members 26a, 26b along the axial direction of the drive shaft 12 can be suppressed, and the mass members 26a, 26b can be set to a desired resonant frequency. Consequently, the vibrations of the drive shaft 12 are reliably attenuated by the tensile/compressive deformation or the shearing deformation (resonance).
According to the present embodiment, at least one of tensile/compressive deformation and shearing deformation occurs on the joint supports 28a, 28b of the dynamic damper 22. If only shearing deformation occurs, then the dimension of the dynamic damper in the longitudinal direction of the drive shaft 12 increases, and if only tensile/compressive deformation occurs, the dimension of the dynamic damper in the diametrical direction of the drive shaft 12 increases. However, the dynamic damper 22 according to the present embodiment has reduced dimensions in both the longitudinal and diametrical directions of the drive shaft 12. Accordingly, the dynamic damper 22 can easily be assembled on the drive shaft 12.
In the above embodiment, the two mass members 26a, 26b are disposed closely to each other (see
In the embodiment shown in
A dynamic damper may be constructed by joining the main body 24 and the mass members 26a, 26b and dispensing with the joint supports 28a, 28b. Alternatively, the joint supports 28a, 28b may be included in the mass members 26a, 26b.
The weights 36a, 36b may have different specific gravities and identical dimensions. The specific gravities may be adjusted by varying the type and amount of a polymeric binder or a metal binder.
A tungsten powder, instead of a tungsten alloy powder, may be used, and a molded body fabricated by a sintering, an MIM process, or a PIM process may be used.
A polymeric binder may be used instead of a metal binder. If a resin binder is used, weights having a specific gravity ranging from about 7 to about 16 are produced. If a rubber binder is used, weights having a specific gravity of about 13 are produced. The relationship between the specific gravity and rigidity of the weight 36a, plotted when the proportions of the polymeric binder and the tungsten alloy are varied to vary the specific gravity of the weight 36a is illustrated in
If a polymeric binder is used, then the specific gravity should preferably range from 9 to 14. The reasons for the specific gravity range are as follows:
For manufacturing the dynamic damper 22, the weight 36a is placed in advance in the cavity 66 of the mold 64 which is constructed of the lower mold 60, the upper mold 62, and the left and right molds 63a, 63b shown in
The relationship between the amount of flexure of the weight 36a which is caused by the pressing force and the specific gravity thereof is illustrated in
If the specific gravity exceeds 14, then the relative amount of the polymeric binder is reduced. Therefore, the tungsten alloy powder or the tungsten powder may not sufficiently be bonded, possibly resulting in a reduction in the strength of the weight 36a.
Preferred examples of the resin binder include nylon resin, polystyrene-based thermoplastic elastomer resin, etc. The weight 36a of this type may be fabricated by an injection molding process or a pressing process.
In the above embodiments, the dynamic dampers 22, 50, 52 with the two mass members 26a, 26b have been described. However, the present invention is not limited to those dynamic dampers. A dynamic damper may have a plurality of, i.e., two or more, mass members.
For example, dynamic dampers 100a through 100f having three mass members 26a through 26c (weights 36a through 36c) and joint supports 28a through 28c according to other embodiments are shown in
In the dynamic dampers 100a through 100f according to the other embodiments, parallel flat surfaces 31 which are held in mutually facing relation are provided between the left mass member 26a and the central mass member 26b and between the central mass member 26b and the right mass member 26c which are disposed along the axial direction of the drive shaft 12. The flat surfaces 31 allow the mold from being opened easily.
Other structural and operational details are the same as those of the dynamic dampers 22, 50, 52 with the two mass members 26a, 26b, and will not be described in detail below.
Number | Date | Country | Kind |
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2005-175410 | Jun 2005 | JP | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/JP2006/306037 | 3/24/2006 | WO | 00 | 12/14/2007 |