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Spinning Out, With Calculus

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steering rack. Stanford University - 5. Dynamic Design Lab. Lanekeeping with Potential Fields ... Tire Force Generation. The contact patch does stick to the ground ... – PowerPoint PPT presentation

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Title: Spinning Out, With Calculus


1
Spinning Out, With Calculus
  • J. Christian Gerdes
  • Associate Professor
  • Mechanical Engineering Department
  • Stanford University

2
Future Vehicles
Clean Multi-Combustion-Mode Engines Control of
HCCI with VVA Electric Vehicle Design
Safe By-wire Vehicle Diagnostics Lanekeeping
Assistance Rollover Avoidance
Fun Handling Customization Variable Force
Feedback Control at Handling Limits
3
Future Systems
  • Change your handling in software
  • Customize real cars like those in a video game
  • Use GPS/vision to assist the driver with
    lanekeeping
  • Nudge the vehicle back to the lane center

4
Steer-by-Wire Systems
  • Like fly-by-wire aircraft
  • Motor for road wheels
  • Motor for steering wheel
  • Electronic link
  • Like throttle and brakes
  • What about safety?
  • Diagnosis
  • Look at aircraft

5
Lanekeeping with Potential Fields
  • Interpret lane boundaries as a potential field
  • Gradient (slope) of potential defines an
    additional force
  • Add this force to existing dynamics to assist
  • Additional steer angle/braking
  • System redefines dynamics of driving but driver
    controls

6
Lanekeeping on the Corvette
7
Lanekeeping Assistance
  • Energy predictions work!
  • Comfortable, guaranteed lanekeeping
  • Another example with more drama

8
P1 Steer-by-wire Vehicle
  • P1 Steer-by-wire vehicle
  • Independent front steering
  • Independent rear drive
  • Manual brakes
  • Entirely built by students
  • 5 students, 15 months from start to first driving
    tests

steering motors
handwheel
9
When Do Cars Spin Out?
  • Can we figure out when the car will spin and
    avoid it?

10
Tires
  • Lets use your knowledge of Calculus to make a
    model of the tire

11
An Observation
  • A tire without lateral force moves in a straight
    line

Tire without lateral force
12
An Observation
  • A tire without lateral force moves in a straight
    line

Tire without lateral force
13
An Observation
  • A tire without lateral force moves in a straight
    line

Tire without lateral force
14
An Observation
  • A tire subjected to lateral force moves
    diagonally

Tire with lateral force
15
An Observation
  • A tire subjected to lateral force moves
    diagonally

Tire with lateral force
16
An Observation
  • A tire subjected to lateral force moves
    diagonally

Tire with lateral force
17
An Observation
  • A tire subjected to lateral force moves
    diagonally

How is this possible? Shouldnt the tire be stuck
to the road?
18
Tire Force Generation
  • The contact patch does stick to the ground
  • This means the tire deforms (triangularly)

19
Tire Force Generation
  • Force distribution is triangular
  • More force at rear
  • Force proportional to slip angle initially
  • Cornering stiffness
  • Force is in opposite direction as velocity
  • Side forces dissipative

a
20
Saturation at Limits
  • Eventually tire force saturates
  • Friction limited
  • Rear part of contact patch saturates first

a
Fy
a
21
Simple Lateral Force Model
x a
x -a
a
  • Deflection initially triangular
  • Defined by slip angle
  • Force follows deflection
  • Assume constant foundation stiffness cpy
  • qy(x) is force per unit length

v(x) (a-x) tana
a
qy(x) cpy(a-x) tana
22
Simple Lateral Force Model
  • Calculate lateral force

x a
x -a
a
v(x) (a-x) tana
a
qy(x) cpy(a-x) tana
Cornering stiffness
23
Tire Forces with Saturation
  • Tire force limited by friction
  • Assume parabolic normal force
    distribution in contact patch

qz(x)
24
Tire Forces with Saturation
  • Tire force limited by friction
  • Assume parabolic normal force
    distribution in contact patch
  • Rubber has two friction coefficients adhesion
    and sliding
  • Lateral force and deflection are friction limited
  • qy(x)

msqz(x)
mpqz(x)
25
Tire Forces with Saturation
  • Tire force limited by friction
  • Assume parabolic normal force
    distribution in contact patch
  • Rubber has two friction coefficients adhesion
    and sliding
  • Lateral force and deflection are friction limited
  • qy(x)
  • Result the rear part of the contact patch is
    always sliding
  • large slip
    small
    slip

msqz(x)
mpqz(x)
26
Calculate Lateral Force
xsl
msqz(x)
mpqz(x)
27
Lateral Force Model
  • The entire contact patch is sliding when a asl
  • The lateral force model is therefore
  • Figures show shape of this relationship

28
Lateral Force Behavior
  • ms1.0 and mp1.0
  • Fiala model

29
Coefficients of Friction
  • Sliding (dynamic friction) ms 0.8
  • Many force-slip plots haveapproximately this
    much friction after the peak, when the tire is
    sliding
  • Seen in previous literature
  • Adhesion (peak friction) mp 1.6
  • Tire/road friction, tested in stationary
    conditions, has been demonstrated to be
    approximately this much
  • Seen in previous literature
  • Model predicts that these values give Fpeak / Fz
    1.0
  • Agrees with expectation

30
Lateral Force with Peak and Slide Friction
  • ms0.8 and mp1.6
  • Peak in curve
  • Can we predict friction on road?

31
Testing at Moffett Field
32
How Early Can We Estimate Friction?
linear
nonlinear
loss of control
33
Ramp Friction Estimates
  • Friction estimated about halfway to the peak
    very early!

linear
nonlinear
loss of control
34
Bicycle Model
  • Outline model
  • How does the vehicle move when I turn the
    steering wheel?
  • Use the simplest model possible
  • Same ideas in video games and car design just
    with more complexity
  • Assumptions
  • Constant forward speed
  • Two motions to figure out turning and lateral
    movement

35
Bicycle Model
  • Basic variables
  • Speed V (constant)
  • Yaw rate r angular velocity of the car
  • Sideslip angle b Angle between velocity and
    heading
  • Steering angle d our input
  • Model
  • Get slip angles, then tire forces, then
    derivatives

36
Calculate Slip Angles
b
a
ar
b
d
V
af
r
ar
d af
37
Vehicle Model
  • Get forces from slip angles (we already did this)
  • Vehicle Dynamics
  • This is a pair of first order differential
    equations
  • Calculate slip angles from V, r, d and b
  • Calculate front and rear forces from slip angles
  • Calculate changes in r and b

38
Making Sense of Yaw Rate and Sideslip
  • What is happening with this car?

39
For Normal Driving, Things Simplify
  • Slip angles generate lateral forces
  • Simple, linear tire model (no spin-outs possible)

a
Fy
40
Two Linear Ordinary Differential Equations
41
Conclusions
  • Engineers really can change the world
  • In our case, change how cars work
  • Many of these changes start with Calculus
  • Modeling a tire
  • Figuring out how things move
  • Also electric vehicle dynamics, combustion
  • Working with hardware is also very important
  • This is also fun, particularly when your models
    work!
  • The best engineers combine Calculus and hardware

42
P1 Vehicle Parameters
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