The present invention relates to estimation of the absolute roll angle of a vehicle body for side airbag deployment and/or brake control, and more particularly to an improved kinematic-based estimation method.
A number of vehicular control systems including vehicle stability control (VSC) systems and rollover detection/prevention systems utilize various sensed parameters to estimate the absolute roll angle of the vehicle body—that is, the angle of rotation of the vehicle body about its longitudinal axis relative to the level ground plane. In addition, knowledge of absolute roll angle is required to fully compensate measured lateral acceleration for the effects of gravity when the vehicle body is inclined relative to the level ground plane.
In general, the absolute roll angle of a vehicle must be estimated or inferred because it cannot be measured directly in a cost effective manner. Ideally, it would be possible to determine the absolute roll angle by simply integrating the output of a roll rate sensor, and in fact most vehicles equipped with VSC and/or rollover detection/prevention systems have at least one roll rate sensor. However, the output of a typical roll rate sensor includes some DC bias or offset that would be integrated along with the portion of the output actually due to roll rate. For this reason, many systems attempt to remove the sensor bias prior to integration. As disclosed in the U.S. Pat. No. 6,542,792 to Schubert et al., for example, the roll rate sensor output can be dead-banded and high-pass filtered prior to integration. While these techniques can be useful under highly transient conditions where the actual roll rate signal is relatively high, they can result in severe under-estimation of roll angle in slow or nearly steady-state maneuvers where it is not possible to separate the bias from the portion of the sensor output actually due to roll rate.
A more effective approach, disclosed in the U.S. Pat. Nos. 6,292,759 and 6,678,631 to Schiffmann, is to form an additional estimate of roll angle that is particularly reliable in slow or nearly steady-state maneuvers, and blend the two roll angle estimates based on specified operating conditions of the vehicle to form the roll angle estimate that is supplied to the VSC and/or rollover detection/prevention systems. In the Shiffmann patents, the additional estimate of roll angle is based on vehicle acceleration measurements, and a coefficient used to blend the two roll angle estimates has a nominal value except under rough-road or airborne driving conditions during which the coefficient is changed to favor the estimate based on the measured roll rate.
Of course, any of the above-mentioned approaches are only as good as the individual roll angle estimates. For example, the additional roll angle estimate used in the above-mentioned Schiffmann patents tends to be inaccurate during turning maneuvers. Accordingly, what is needed is a way of forming a more accurate estimate of absolute roll angle.
The present invention provides an improved method of estimating the absolute roll angle of a vehicle body under any operating condition, including normal driving, emergency maneuvers, driving on banked roads and near rollover situations. The roll angle estimate is based on typically sensed parameters, including roll rate, lateral acceleration, yaw rate, vehicle speed, and optionally, longitudinal acceleration. Roll rate sensor bias is identified by comparing the sensed roll rate with roll rate estimates inferred from other measured parameters for fast and accurate removal of the bias. A first preliminary estimate of roll angle, generally reliable in nearly steady-state conditions, is determined from a kinematic relationship involving lateral acceleration, yaw rate and vehicle speed. The final or blended estimate of roll angle is then determined by blending the preliminary estimate with a second preliminary estimate based on the bias-corrected measure of roll rate. In the blending process, the relative weighting between two preliminary roll angle estimates depends on their frequency and on the driving conditions so that the final estimate continuously favors the more accurate of the preliminary estimates. The blended estimate is used for several purposes, including estimating the lateral velocity and side-slip angle of the vehicle.
Referring to
If the roll rate w of vehicle 10 about its longitudinal axis is measured, an estimate φe
where t denotes time and ωm is the measured roll rate. Unfortunately, the output of a typical roll rate sensor includes some bias error that would be integrated along with the portion of the output actually due to roll rate. Thus, pure integration of the measured roll rate has infinite sensitivity to the bias error because the error is integrated over time. When dead-banding and high-pass (i.e., wash-out) filtering are used to compensate for the bias error, there is still a conflict between the immunity to bias and the ability to track slowly-varying (or constant) roll angles because the bias compensation also reduces the portion of the signal actually due to roll rate. As a result, a roll angle estimate based on roll rate integration is reasonably good during quick transient maneuvers, but less accurate during slow maneuvers or in nearly steady-state conditions when the roll angle changes slowly. As explained below, one aspect of the present invention is directed to an improved method of compensating for the bias error in a measured roll rate signal without substantially diminishing the portion of the signal actually due to roll rate.
An alternative way of determining the total roll angle θ is to consider it in the context of the kinematic relationship:
a
ym
={dot over (v)}
y
+v
x
Ω−g sin φ (2)
where vy is the lateral velocity of vehicle center-of-gravity, vx is the vehicle longitudinal velocity, Ω is vehicle yaw rate, and g is the acceleration of gravity (9.806 m/s2). The sign convention used in equation (2) assumes that lateral acceleration aym and yaw rate Ω are positive in a right turn, but the roll angle φ due to the turning maneuver is negative.
During nearly steady-state conditions, the derivative of lateral velocity (i.e., {dot over (v)}y) is relatively small, and an estimate φek of the roll angle φ can be obtained by ignoring {dot over (v)}y and solving equation (2) for 0 as follows:
The longitudinal velocity vx, the yaw rate Ω, and the lateral acceleration aym can be measured, and g is simply a gravitational constant as mentioned above. Thus, a reasonably good estimate φek of roll angle φ under nearly steady-state conditions may be easily calculated. However, the accuracy of the estimate φek deteriorates in transient maneuvers where the derivative of lateral velocity is non-negligible.
In summary, the foregoing methods of estimating absolute roll angle each have significant limitations that limit their usefulness. As explained above, a roll angle estimate based on roll rate integration is reasonably good during quick transient maneuvers, but less accurate during slow maneuvers or in nearly steady-state conditions when roll angle changes slowly due to inability to separate the bias error from the portion of the signal actually due to roll rate. On the other hand, the roll angle estimate φek based on the kinematic relationship of equations (2) and (3) is reasonably good during nearly steady-state (low frequency) maneuvers, but unreliable during transient (high frequency) maneuvers.
It can be seen from the above that the two roll angle estimation methods are complementary in that conditions that produce an unreliable estimate from one estimation method produce an accurate estimate from the other estimation method, and vice versa. Accordingly, the method of this invention blends both estimates in such a manner that the blended roll angle estimate is always closer to the initial estimate that is more accurate.
Block 42 pertains to systems that include a sensor 30 for measuring longitudinal acceleration axm, and functions to compensate the measured roll rate ωm
a
xm
={dot over (v)}
x
−v
y
Ω+g sin θ (4)
where axm is the measured longitudinal acceleration, {dot over (v)}x is the time rate of change in longitudinal speed vx, vy is the vehicle's side-slip or lateral velocity, Ω is the measured yaw rate, and g is the acceleration of gravity. Equation (4) can be rearranged to solve for pitch angle θ as follows:
The term {dot over (v)}x is obtained by differentiating (i.e., high-pass filtering) the estimated vehicle speed vx. If the lateral velocity vy is not available, the product (vyΩ) can be ignored because it tends to be relatively small as a practical matter. However, it is also possible to use a roll angle estimate to estimate the lateral velocity vy, and to feed that estimate back to the pitch angle calculation, as indicated by the dashed flow line 60. Also, the accuracy of the pitch angle calculation can be improved by magnitude limiting the numerator of the inverse-sine function to a predefined threshold such as 4 m/s2. The magnitude-limited numerator is then low-pass filtered with, for example, a second-order filter of the form bnf2/(s2+2ζbnf+bnf2), where bnf is the undamped natural frequency of the filter and ζ is the damping ratio (example values are bnf=3 rad/sec and ζ=0.7). Also, modifications in the pitch angle calculation may be made during special conditions such as heavy braking when the vehicle speed estimate vx may be inaccurate. In any event, the result of the calculation is an estimated pitch angle θe, which may be subjected to a narrow dead-zone to effectively ignore small pitch angle estimates. Of course, various other pitch angle estimation enhancements may be used, and additional sensors such as a pitch rate sensor can be used to estimate θ.
Once the pitch angle estimate θe is determined, the measured roll rate is corrected by adding the product of the yaw rate Ω and the tangent of the pitch angle θe to the measured roll rate ∫m
ωm=ωm
Since in nearly all cases, the pitch angle θe is less than 20° or so, equations (5) and (6) can be simplified by assuming that sin θ≅tan θ≅θ. And as mentioned above, the measured roll rate ωm
Block 44 is then executed to convert the measured roll rate signal dim into a bias-compensated roll rate signal ωm
A first roll rate estimate ωeay is obtained by using the relationship:
φeay=−Rgainaym (7)
to calculate a roll angle Ota corresponding to the measured lateral acceleration aym, and differentiating the result. The term Rgain in equation (7) is the roll gain of vehicle 10, which can be estimated for a given vehicle as a function of the total roll stiffness of the suspension and tires, the vehicle mass, and distance from the road surface 12 to the vehicle's center-of-gravity. However, the measured lateral acceleration aym is first low-pass filtered to reduce the effect of measurement noise. Preferably, the filter is a second-order filter of the form bnf2/(s2+2ζbnf+bnf2), where bnf is the un-damped natural frequency of the filter and ζ is the damping ratio (example values are bnf=20 rad/s and ζ=0.7). And differentiation of the calculated roll angle φeay is achieved by passing φeay through a first-order high-pass filter of the form bfs/(s+bf), where bf is the filter cut off frequency (an example value is bf=20 rad/sec).
A second roll rate estimate ωek is obtained by using equation (3) to calculate a roll angle φek and differentiating the result. The derivative of lateral velocity, {dot over (v)}y, is neglected since near steady-state driving conditions are assumed. Algebraically, φek is given as:
As indicated in the above equation, the numerator (vxΩ−aym) of the inverse sine function is also low-pass filtered, preferably with the same form of filter used for the aym in the preceding paragraph. As a practical matter, the inverse sine function can be omitted since the calculation is only performed for small roll angles (less than 3° or so). Differentiation of the calculated roll angle φek to produce a corresponding roll rate ωek is achieved in the same way as described for roll angle φeay in the preceding paragraph.
Once the roll rate estimates ωeay and ωek have been calculated, a number of tests are performed to determine their stability and reliability. First, the absolute value of each estimate must be below a threshold value for at least a predefined time on the order of 0.3-0.5 sec. Second, the absolute value of their difference (that is, |ωeay−ωek|) must be below another smaller threshold value for at least a predefined time such as 0.3-0.5 sec. And finally, the absolute value of the difference between the measured lateral acceleration and the product of yaw rate and vehicle speed (that is, |aym−vxΩ|) must be below a threshold value such as 1 m/sec2 for at least a predefined time such as 0.3-0.5 sec. Instead of requiring the conditions to be met for a predefined time period, it is sufficient to require that the rate-limited versions of these signals satisfy specified conditions.
When the above conditions are all satisfied, the roll rate estimates ωeay and ωek are deemed to be sufficiently stable and reliable, and sufficiently close to each other, to be used for isolating the roll rate sensor bias error. In such a case, inconsistencies between the estimated roll rates and the measured roll rate are considered to be attributable to roll rate sensor bias error. First, the difference Δωm
ωbias(ti+1)=(1−bΔt)ωbias(ti)+bΔtΔωm
where ti+1 denotes the current value, ti denotes a previous value, b is the filter cut off frequency (0.3 rad/sec, for example), and Δt is the sampling period. The initial value of ωbias (that is, ωbias (t0)) is either zero or the value of ωbias from a previous driving cycle. The roll rate bias error ωbias is periodically updated so long as the stability and reliability conditions are met, but updating is suspended when one or more of the specified conditions is not satisfied. As a practical matter, updating can be suspended by setting b=0 in equation (9) so that ωbias(ti+1)=ωbias(ti). Finally, the calculated bias error ωbias is subtracted from the measured roll rate ωm, yielding the corrected roll rate ωm
The block 46 is then executed to determine the roll angle estimate from a kinematic relationship using measured lateral acceleration, yaw rate and estimated vehicle speed. Fundamentally, the estimate of roll angle is obtained from equation (3), but with additional processing of the numerator term (vxΩ−aym) of the inverse sine function. The value of the numerator term is determined and then limited in magnitude to a threshold value athresh such as 5 m/sec2; the limiting serves to reduce error due to the neglected derivative of lateral velocity when it is large, as may occur during very quick transient maneuvers. The limited difference (vxΩ−aym)lim is then passed through a low pass filter to attenuate the effect of noise; for example, the filter may be a second order filter of the form bnf2/(s2+2ζbnf+bnf2) where bnf is the undamped natural frequency of the filter and ζ is the damping ratio (example values are bnf=3 rad/sed and ζ=0.7). The filter output (vxΩ−aym)lim
Block 48 is then executed to determine a blended estimate φebl of the total roll angle φ by blending φek with a roll angle determined by integrating the bias-compensated roll rate measurement ωm
{dot over (φ)}ebl+bbl
Representing equation (11) in the Laplace domain, and solving for the blended roll angle estimate φebl yields:
which in practice is calculated on a discrete-time domain basis as follows:
φebl(ti+1)=(1−bbl
where ti+1 denotes the current value, ti denotes a previous value, and Δt is the sampling period. If the roll angle obtained by integrating ωm
In this form, it is evident that the blended roll angle estimate φebl is a weighted sum of φek and φw, with the weight dependent on the frequency of the signals (designated by the Laplace operand “s”) so that the blended estimate φebl is always closer to the preliminary estimate that is most reliable at the moment. During steady-state conditions, the body roll rate is near-zero and the signal frequencies are also near-zero. Under such steady-state conditions, the coefficient of φek approaches one and the coefficient of φw approaches zero, with the result that φek principally contributes to φebl. During transient conditions, on the other hand, the body roll rate is significant, and the signal frequencies are high. Under such transient conditions, the coefficient of φek approaches zero and the coefficient of φw approaches one, with the result that φw principally contributes to φebl. The change between these two extreme situations is gradual and the transition depends on the value of blending factor bbl
The blending factor bbl
According to a preferred embodiment, the presence of a nearly steady-state condition is detected when a set of three predefined conditions have been met for a specified period of time such as 0.5 seconds. First, the magnitude of the bias-compensated roll rate (i.e., |ωm
Block 50 is then executed to compensate the measured lateral acceleration ay, for the gravity component due to roll angle. The corrected lateral acceleration aycor is given by the sum (aym+g sin φebl), where φebl is the blended roll angle estimate determined at block 48. The corrected lateral acceleration aycor can be used in conjunction with other parameters such as roll rate and vehicle speed for detecting the onset of a rollover event.
Finally, block 52 is executed to use the blended roll angle estimate φebl to estimate other useful parameters including the vehicle side slip (i.e., lateral) velocity vy and side-slip angle β. The derivative of lateral velocity can alternately be expressed as (ay−vxΩ) or (aym+g sin φ−vxΩ), where ay in the expression (ay−vxΩ) is the actual lateral acceleration, estimated in block 50 as corrected lateral acceleration aycor. Thus, derivative of lateral velocity may be calculated using aycor for ay in the expression (ay−vxΩ), or using the blended roll angle estimate φebl for φ in the expression (aym+g sin φ−vxΩ). Integrating either expression then yields a reasonably accurate estimate vye of side slip velocity vy, which can be supplied to block 42 for use in the pitch angle calculation, as indicated by the broken flow line 60. And once the side-slip velocity estimate Vye has been determined, the side-slip angle β at the vehicle's center of gravity is calculated as:
In summary, the present invention provides a novel and useful way of accurately estimating the absolute roll angle of a vehicle body under any vehicle operating condition by blending two preliminary estimates of roll angle according to their frequency. A first preliminary roll angle estimate based on the measured roll rate is improved by initially compensating the roll rate signal for bias error using roll rate estimates inferred from other measured parameters. And a second preliminary roll angle estimate is determined based on the kinematic relationship among roll angle, lateral acceleration, yaw rate and vehicle speed. The blended estimate of roll angle utilizes a blending coefficient that varies with the frequency of the preliminary roll angle signals so that the blended estimate continuously favors the more accurate of the preliminary roll angle estimates, and a blending factor used in the blending coefficient is set to different values depending whether the vehicle is in a steady-state or transient condition. The blended estimate is used to estimate the actual lateral acceleration, the lateral velocity and side-slip angle of the vehicle, all of which are useful in applications such as rollover detection and vehicle stability control.
While the present invention has been described with respect to the illustrated embodiment, it is recognized that numerous modifications and variations in addition to those mentioned herein will occur to those skilled in the art. For example, the some or all of equations be characterized as look-up tables to minimize computation requirements, and trigonometric functions may be approximated by their Fourier expansion series. Also, the lateral velocity may be determined using a model-based (i.e., observer) technique with the corrected lateral acceleration aycor as an input, instead of integrating the estimated derivative of lateral velocity. Finally, it is also possible to apply the blending method of this invention to estimation of absolute pitch angle θ in systems including a pitch rate sensor; in that case, a first preliminary pitch angle estimate would be obtained by integrating a bias-compensated measure of the pitch rate, and a second preliminary pitch angle estimate would be obtained from equation (5). Of course, other modifications and variations are also possible. Accordingly, it is intended that the invention not be limited to the disclosed embodiment, but that it have the full scope permitted by the language of the following claims.