In one embodiment, a pressurized top mount for a vehicle, with a bracket configured to be attached to the body of the vehicle, is disclosed that comprises: a chamber attached to one of the body or the bracket, configured to slidably receive an end of a piston rod of a suspension component, and a pressurized fluid volume contained in the chamber, configured to apply a force to the end of the piston rod.
Modern vehicles generally include a suspension system that couples a body of the vehicle to one or more wheels of the vehicle. The suspension system may attach to the vehicle body via a set of top mount assemblies that are located near each wheel of the vehicle. As active suspension systems become commercially viable, there is a need for top mounts designed to be compatible with such active suspension systems.
In a suspended vehicle, a top mount assembly may be utilized to physically attach a body of the vehicle to a rod (e.g., a piston rod) of a suspension component of the vehicle. In an active suspension system, the suspension component may be a hydraulic actuator; while in a passive suspension system, the suspension component may be a hydraulic damper. The inventors have recognized that in an active suspension system that includes a hydraulic actuator, under static conditions the hydraulic actuator may apply static forces to the top mount assembly that greatly exceed static forces conventionally associated with a damper of a passive suspension system. In an active suspension system, these static forces may approach or even exceed the designed operating limits for the top mount assembly. As a result, top mount assemblies that perform well in passive suspension systems may suffer from significant performance degradation when utilized in active suspension systems. The inventors have recognized that, for active suspension systems, performance of the top mount assembly (and, therefore, performance of the overall suspension system) may be augmented by counter-balancing the static forces applied by the hydraulic actuator. For example, in certain embodiments, a fluid-filled volume may be located such that fluid in the volume applies a force to the rod of the hydraulic actuator that partially or fully balances the static forces associated with the hydraulic actuator.
Spring constants of each of the spring elements 5a-d may be combined using equations known in the art to determine a single, combined spring constant. For example, a set of n spring elements oriented in a parallel arrangement may be characterized by a single combined spring element using the equation kcombined=k1+k2+k3+ . . . +kn, where kcombined represents the combined spring constant and k1, k2, k3, kn represent a respective spring constant of spring elements 1, 2, 3, and n. Likewise, a set of n spring elements oriented in a series arrangement may be characterized by a single combined spring element using the equation (kcombined)−1=(k1)−1+(k2)−1+(k3)−1 . . . +(kn)−1. As would be recognized by one of ordinary skill in the art, these equations may be modified appropriately such that any set of spring elements oriented in any manner may be characterized by a single combined spring constant and/or a combined compliance. In certain embodiments, a combined spring constant and/or a combined compliance provided by the set of spring elements 5a-d may be tuned to attenuate transmission of noise and/or high frequency vibrations (e.g. generated by road excitation) from the wheel 8 to the vehicle body 9 and/or cabin.
A “neutral position” 11 of the strike plate 4 refers to the position of the strike plate 4, relative to the bracket 3, when the combined force applied by the set of spring elements 5a-d is equal in magnitude and opposite in direction to the weight of the strike plate 4. The strike plate may be in its neutral position 11 when either (a) the rod 6 is not attached to the top mount assembly, or (b) the rod 6 is attached but does not apply any force to the strike plate 4. A force applied by the rod 6 onto the strike plate 4 may cause a position of the strike plate 4 to vary relative to its neutral position 11, thereby causing compression or extension of certain spring elements 5a-5d.
In certain embodiments, the combined spring constant provided by the set of spring elements may progressively increase as the strike plate 4 is increasingly displaced relative to its neutral position 11. An example of such behavior is shown in
The first surface 302 of the piston may be exposed to fluid having a first pressure (designated P1), while the second surface 304 of the piston may be exposed to fluid having a second pressure. Due to the piston rod 6, a first area (denoted A1 herein) of the first surface 302 that is exposed to fluid in the first volume 306 may be greater than a second area (denoted A2 herein) of the second surface 304 that is exposed to fluid in the second volume 308. Since force is equal to the product of pressure times area (i.e., F=P*A), fluid in the first volume 306 applies a first force (designated F1) to the first surface 302 of the piston; this first force has a magnitude equal to F1=P1*A1. Likewise, fluid in the second volume 308 applies a second force (designated F2) to the second surface 302 of the piston; this second force has a magnitude F2=P2*A2. The net force applied on the piston is equal to the difference between the first force and the second force (i.e., Fnet=F1−F2), and is given mathematically by equation 1.
Fnet=F1−F2=P1*A1−P2*A2 Equation 1
A “static condition” is understood to refer to conditions when there is a net zero flow of fluid between the first volume 306 and the second volume 308; such net zero flow occurs when the first pressure (P1) of fluid in the first volume 306 is equal to the second pressure (P2) of fluid in the second volume 308. In an active suspension system, static conditions may be achieved when the pump is inactive (e.g., when the pump does not generate a pressure differential). As can be seen from equation 1, even under a static condition of the suspension component (i.e., even when P1=P2), a net force may be applied to the piston due to the difference between the first area (A1) and the second area (A2). The net static force applied to the piston 300 under static conditions of the suspension component is given by equation 2, where Pstatic=P1=P2.
Fnet,static=Pstatic*(A1−A2) Equation 2
When the suspension component is attached to the top mount assembly via the piston rod 6, the net static force (Fnet,static) applied to the piston 300 may be transferred through the piston rod 6 to the strike plate 4. Application of the net static force to the strike plate may cause the strike plate to move away from its neutral position to a loaded position. A “loaded position” of the strike plate 4 is understood to refer to the position of the strike plate 4, relative to the bracket 3, when the net static force is applied to the strike plate 4 by the rod of the suspension component under static conditions. Due to the net static force, the loaded position of the strike plate 4 may be displaced relative to the neutral position 11 of the strike plate 4. The difference between the loaded position of the strike plate 4 and the neutral position 11 of the strike plate 4 may be referred to as static displacement, and depends on the static pressure (Pstatic) of fluid in the first and second volumes. For sufficiently high static pressures, such as those utilized in active suspensions, the static displacement may lie at a point along the curve shown in
In light of the above, the inventors have recognized that, especially for active suspensions that experience high static pressures, it may be advantageous to utilize a top mount assembly configured such that static displacement of the strike plate 4 in the top mount is minimized.
As illustrated in
In certain embodiments, as shown in
Alternatively, in certain embodiments as illustrated by the exemplary suspension system of
In the illustrated embodiment, when the pump is inactive (e.g., when there is no pressure differential across the pump), the first pressure of fluid in the first volume of the suspension component may be equal to the second pressure of fluid in the second volume of the suspension component—that is, when the pump is inactive, the suspension component may be under static conditions (i.e., P1=P2=Pstatic). Since the first volume and/or second volume are in fluid communication with the liquid filled volume of the accumulator, fluid pressure in the liquid filled volume of the accumulator may equilibrate such that a fourth pressure of fluid in the liquid filled volume is equal to the first pressure and second pressure (e.g., under static conditions, P4=P1=P2=Pstatic). Further, due to the slidable nature of the piston, fluid pressure in the gas filled volume of the accumulator may equilibrate such that a fifth pressure of fluid in the gas filled volume of the accumulator is equal to the fourth pressure in the liquid filled volume of the accumulator (e.g., under static conditions, P5=P4=P1=P2) of fluid in the liquid filled volume of the accumulator. Finally, due to fluid communication between the third volume of the top mount assembly and the gas filled volume of the accumulator, fluid pressure in the third volume may equilibrate such that the third pressure of fluid in the third volume is equal to the fourth pressure of fluid in the gas filled volume of the accumulator (e.g., under static conditions, P3=P5=P4=P1=P2). Fluid in the third volume of the top mount assembly may therefore apply a force to the piston rod that fully, nearly fully, or at least partially counterbalances the net static force applied on the piston. The force applied by fluid in the third volume may dynamically vary with changes in the net static force that occur due to temperature changes of fluid in the first volume, second volume, or accumulator volumes
In certain embodiments, a tuned restriction may be located between gas filled volume of the accumulator and the third volume of the top mount. This restriction may serve to mitigate transmission of high-frequency pressure ripple from the pump into the third volume of the top mount. As used herein, high-frequency may be any predefined frequency range, for example frequencies in the range of 5-1000 Hz, 10-1000 Hz, 15-1000 Hz, or 20-1000 Hz.
Alternatively or additionally, in certain embodiments, the third volume of the top mount assembly may be in fluid communication with at least one of the first volume of the suspension component and the second volume of the suspension component. Such fluid communication from the suspension component to the third volume of the top mount may occur, for example, by a passage way that runs through the piston rod. In these embodiments, the third volume may be at least partially filled with a non-compressible fluid (e.g., oil).
In certain embodiments, the third volume of the top mount assembly may be at least partially filled with a compressible fluid (e.g., a gas) and the first volume and second volume of the suspension component may be at least partially filled with a non-compressible fluid (e.g., oil). In these embodiments, a diaphragm may be utilized to separate or effectively separate the compressible fluid (e.g., the gas) in the third volume of the top mount assembly from the non-compressible fluid (e.g., the oil) in at least one of the first volume and second volume of the suspension component. In certain embodiments, the diaphragm may be sufficiently flexible such that a change in pressure of the non-compressible fluid in at least one of the first volume and second volume of the suspension component thereby results in a similar change in pressure of the compressible fluid in the third volume of the top mount.
In certain embodiments, the third volume may be partially filled with a compressible fluid and partially filled with a non-compressible fluid. In these embodiments, a diaphragm or a piston may be utilized to separate or effectively separate the compressible fluid in the third volume from the non-compressible fluid in the third volume. In these embodiments the non-compressible fluid in the third volume may be in fluid communication with at least one of the first volume and second volume of the suspension component. Under static conditions the third volume may counteract the net static force, and the pressure of the non-compressible fluid in the third volume may be equal to or effectively equal to the pressure in at least one of the first volume and second volume of the suspension component. Furthermore, in these embodiments, a fluid restriction may be fluidly disposed between the non-compressible fluid in the third volume and at least one of the first volume and second volume of the suspension component. This restriction may serve to mitigate transmission of high-frequency pressure ripple from the first or second volume to the third volume.
This application claims the benefit under 35 U.S.C. § 119(e) of U.S. provisional application Ser. No. 62/569,072, filed Oct. 6, 2017, the disclosure of which is incorporated by reference in its entirety.
Number | Date | Country | |
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62569072 | Oct 2017 | US |