Not Applicable.
1. Field of the Invention
The present invention relates in general to a method for providing a corrective action to reduce an actual rollover, and more specifically, for a method of applying brake controls to reduce an actual rollover without altering the vehicle trajectory.
2. Description of the Related Art
A vehicle typically becomes unstable (over steered) before it starts to roll over. Dynamic stability control systems are utilized in vehicles to prevent the roll over by reducing the tendency of the over steering. Known methods attempt to prevent a vehicle rollover event from occurring by reducing the speed of the vehicle through braking and/or modifying the vehicle trajectory. While changing the vehicle trajectory may mitigate a potential vehicle rollover event, such trajectory changes may be an undesirable control due to surrounding conditions (e.g., obstacles). With respect to vehicle braking, applying all vehicle brakes in an anti-lock brake mode will reduce the vehicle speed and counteract the potential vehicle rollover event, but it may also result in undesirable vehicle trajectory changes.
The present invention has the advantage of reducing the roll moment in a rollover event by producing a longitudinal slip on an outside wheel through vehicle braking control.
In one aspect of the invention, a method is provided for counteracting a roll moment in a vehicle rollover event. A potential occurrence of the rollover event is detected over an outside wheel. The potential rollover occurrence event is detected when a tire lateral force is greater than a lateral acceleration force. A braking torque is applied to at least one outside wheel for producing a longitudinal wheel slip on the at least one outside wheel wherein the longitudinal wheel slip increases a longitudinal force acting on the at least one outside wheel. The peak lateral friction is reduced between a tire coupled to the at least one outside wheel and an underlying road surface in order to reduce the peak lateral friction and the roll moment.
Referring now to the Drawings and particularly to
At or near the point of rollover, the normal and lateral forces of the inside tires 24 are negligible. Therefore, it is assumed that the vehicle inertia forces are balanced by the reaction forces of the outside tires 22. The vehicle lateral acceleration force (aym) 38 (i.e., inertia force) is balanced by the tire lateral force Fy. The tire lateral force Fy is equal to the product of the friction (of the tire and road surface) and a gravitational force 30 of the vehicle 10 so long as the tire friction remains below a saturation limit that is tolerated by a road surface condition. This is represented by the following formula:
Fy=μmg
where μ is tire lateral friction coefficient, m is a vehicle total mass, and g is a gravity constant. The tire lateral friction coefficient μ is a function of tire longitudinal slip as well as tire lateral slip. The saturation limit is reduced when the tire longitudinal slip increases. Tire longitudinal slip occurs for a respective wheel when a sufficiently large braking force is applied to the respective wheel.
In the present invention, braking pressure applied to each respective wheel is independently controlled so that a respective braking force may be applied to a respective wheel independent of the other wheels. This creates a slip condition only on the respective braking wheel for reducing the roll moment in preventing the rollover event.
M=R×F
x
where R is a vector connecting the C.G. 32 to the outside tire 22, and Fx is the tire longitudinal force. As shown in
ΔFy*h
where ΔFy is defined as an amount of reduced lateral force associated with the tire longitudinal slip, and h is defined as a nominal C.G. height of the vehicle. The larger the ΔFy, the lower the force of the moment acting upon the vehicle to produce the vehicle rollover.
In a second preferred embodiment, a respective force may be applied only to the rear outside wheel (not shown) or in addition to the braking force applied to the front outside wheel 22. It is known that forces Fx and Fy induce a moment about the z-axis (i.e., yaw moment) resulting in a potential trajectory change. However by applying braking pressure to the front and rear wheel appropriately, the amount of the induced yaw moment may be minimized. For example, forces Fx and ΔFy on the rear outside wheel induces yaw moments whereby the signs of the forces are opposite which results in a negligible yaw moment. Forces Fx and ΔFy on the front wheels have a same sign which may result in a significant yaw moment. Although these forces exerted on the front wheels may create a yaw disturbance, such disturbances may potentially correct an oversteering condition that minimizes the overall trajectory effects on the vehicle yaw stability dynamics.
This application claims benefit to U.S. Provisional Application Ser. No. 60/604,776, filed Aug. 26, 2004, the disclosure of which is incorporated herein by reference.
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/US05/29912 | 8/22/2005 | WO | 00 | 5/15/2008 |
Number | Date | Country | |
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60604776 | Aug 2004 | US |