Cruise control

This page documents the cruise control system that is used as a running example throughout the text. A detailed description of the dynamics of this system are presented in Chapter 4 - Examples. This page contains a description of the system, including the models and commands used to generate some of the plots in the text.

Note: the Python code on this page makes use of the Python Control Systems Library, an open source software toolbox for control systems analysis.

Introduction

Cruise control is the term used to describe a control system that regulates the speed of an automobile. Cruise control was commercially introduced in 1958 as an option on the Chrysler Imperial. The basic operation of a cruise controller is to sense the speed of the vehicle, compare this speed to a desired reference, and then accelerate or decelerate the car as required. The figure to the right shows a block diagram of this feedback system.

A simple control algorithm for controlling the speed is to use a "proportional plus integral" feedback. In this algorithm, we choose the amount of gas flowing to the engine based on both the error between the current and desired speed, and the integral of that error. The plot on the right shows the results of this feedback for a step change in the desired speed and a variety of different masses for the car (which might result from having a different number of passengers or towing a trailer). Notice that independent of the mass (which varies by 25% of the total weight of the car), the steady state speed of the vehicle always approaches the desired speed and achieves that speed within approximately 10-15 seconds. Thus the performance of the system is robust with respect to this uncertainty.

Dynamic model

To develop a mathematical model we start with a force balance for the car body. Let $v$ be the speed of the car, $m$ the total mass (including passengers), $F$ the force generated by the contact of the wheels with the road, and $F_{\text{d}}$ the disturbance force due to gravity, friction and aerodynamic drag. The equation of motion of the car is simply

$m{\frac {dv}{dt}}=F-F_{\text{d}}.$

The force $F$ is generated by the engine, whose torque is proportional to the rate of fuel injection, which is itself proportional to a control signal $0\leq u\leq 1$ that controls the throttle position. The torque also depends on engine speed $\omega$. A simple representation of the torque at full throttle is given by the torque curve

$T(\omega )=T_{\text{m}}\left(1-\beta {\biggl (}{\frac {\omega }{\omega _{\text{m}}}}-1{\biggr )}^{2}\right),$

where the maximum torque $T_{\text{m}}$ is obtained at engine speed $\omega _{\text{m}}$. Typical parameters are $T_{m}=190$ Nm, $\omega _{m}$ = 420 rad/s (about 4000 RPM) and $\beta =0.4$.

Let $n$ be the gear ratio and $r$ the wheel radius. The engine speed is related to the velocity through the expression

$\omega ={\frac {n}{r}}v=:\alpha _{n}v,$

and the driving force can be written as

$F={\frac {nu}{r}}T(\omega )=\alpha _{n}uT(\alpha _{n}v).$

Typical values of $\alpha _{n}$ for gears 1 through 5 are $\alpha _{1}=40$, $\alpha _{2}=25$, $\alpha _{3}=16$, $\alpha _{4}=12$ and $\alpha _{5}=10$. The inverse of $\alpha _{n}$ has a physical interpretation as the effective wheel radius. The figure to the right shows the torque as a function of vehicle speed. The figure shows that the effect of the gear is to "flatten" the torque curve so that an almost full torque can be obtained almost over the whole speed range.

The disturbance force $F_{\text{d}}$ has three major components: $F_{\text{g}}$, the forces due to gravity; $F_{\text{r}}$, the forces due to rolling friction; and $F_{\text{a}}$, the aerodynamic drag. Letting the slope of the road be $\theta$, gravity gives the force $F_{\text{g}}=mg\sin \theta$, where $g=9.8\,{\text{m}}/{\text{s}}^{2}$ is the gravitational constant. A simple model of rolling friction is

$F_{\text{r}}=mgC_{\text{r}}\,{\text{sgn}}(v),$

where $C_{\text{r}}$ is the coefficient of rolling friction and sgn($v$) is the sign of $v$ or zero if $v=0$. A typical value for the coefficient of rolling friction is $C_{\text{r}}=0.01$. Finally, the aerodynamic drag is proportional to the square of the speed:

$F_{\text{a}}={\frac {1}{2}}\rho C_{\text{d}}Av^{2},$

where $\rho$ is the density of air, $C_{d}$ is the shape-dependent aerodynamic drag coefficient and $A$ is the frontal area of the car. Typical parameters are $\rho =$ 1.3 k/m${}^{3}$, $C_{\text{d}}=0.32$ and $A=$ 2.4 m${}^{2}$.

Python code

The model for the system above can be built using the Python Control Toolbox. The code blocks in this section can be used to generate the plots above.

Package initialization

import numpy as np
import matplotlib as mpl
import matplotlib.pyplot as plt
from math import pi
import control as ct

Vehicle model

def vehicle_update(t, x, u, params={}):
    """Vehicle dynamics for cruise control system.

    Parameters
    ----------
    x : array
         System state: car velocity in m/s
    u : array
         System input: [throttle, gear, road_slope], where throttle is
         a float between 0 and 1, gear is an integer between 1 and 5,
         and road_slope is in rad.

    Returns
    -------
    float
        Vehicle acceleration
    """

    from math import copysign, sin
    sign = lambda x: copysign(1, x)         # define the sign() function
    
    # Set up the system parameters
    m = params.get('m', 1600.)              # vehicle mass, kg
    g = params.get('g', 9.8)                # gravitational constant, m/s^2
    Cr = params.get('Cr', 0.01)             # coefficient of rolling friction
    Cd = params.get('Cd', 0.32)             # drag coefficient
    rho = params.get('rho', 1.3)            # density of air, kg/m^3
    A = params.get('A', 2.4)                # car area, m^2
    alpha = params.get(
        'alpha', [40, 25, 16, 12, 10])      # gear ratio / wheel radius

    # Define variables for vehicle state and inputs
    v = x[0]                           # vehicle velocity
    throttle = np.clip(u[0], 0, 1)     # vehicle throttle
    gear = u[1]                        # vehicle gear
    theta = u[2]                       # road slope

    # Force generated by the engine
    omega = alpha[int(gear)-1] * v      # engine angular speed
    F = alpha[int(gear)-1] * motor_torque(omega, params) * throttle

    # Disturbance forces
    #
    # The disturbance force Fd has three major components: Fg, the forces due
    # to gravity; Fr, the forces due to rolling friction; and Fa, the
    # aerodynamic drag.

    # Letting the slope of the road be \theta (theta), gravity gives the
    # force Fg = m g sin \theta.
    Fg = m * g * sin(theta)

    # A simple model of rolling friction is Fr = m g Cr sgn(v), where Cr is
    # the coefficient of rolling friction and sgn(v) is the sign of v (±1) or
    # zero if v = 0.
    Fr  = m * g * Cr * sign(v)

    # The aerodynamic drag is proportional to the square of the speed: Fa =
    # 1/2 \rho Cd A |v| v, where \rho is the density of air, Cd is the
    # shape-dependent aerodynamic drag coefficient, and A is the frontal area
    # of the car.
    Fa = 1/2 * rho * Cd * A * abs(v) * v
    
    # Final acceleration on the car
    Fd = Fg + Fr + Fa
    dv = (F - Fd) / m
    
    return dv

Engine model

def motor_torque(omega, params={}):
    # Set up the system parameters
    Tm = params.get('Tm', 190.)             # engine torque constant
    omega_m = params.get('omega_m', 420.)   # peak engine angular speed
    beta = params.get('beta', 0.4)          # peak engine rolloff

    return np.clip(Tm * (1 - beta * (omega/omega_m - 1)**2), 0, None)

Input/output model for the vehicle system

vehicle = ct.NonlinearIOSystem(
    vehicle_update, None, name='vehicle',
    inputs = ('u', 'gear', 'theta'), outputs = ('v'), states=('v'))

Input/output torque curves (plot)

# Figure 4.2a - single torque curve as function of omega
omega_range = np.linspace(0, 700, 701)
plt.subplot(2, 2, 1)
plt.plot(omega_range, [motor_torque(w) for w in omega_range])
plt.xlabel('Angular velocity $\omega$ [rad/s]')
plt.ylabel('Torque $T$ [Nm]')
plt.grid(True, linestyle='dotted')

# Figure 4.2b - torque curves in different gears, as function of velocity
plt.subplot(2, 2, 2)
v_range = np.linspace(0, 70, 71)
alpha = [40, 25, 16, 12, 10]
for gear in range(5):
    omega_range = alpha[gear] * v_range
    plt.plot(v_range, [motor_torque(w) for w in omega_range],
             color='blue', linestyle='solid')

# Set up the axes and style
plt.axis([0, 70, 100, 200])
plt.grid(True, linestyle='dotted')

# Add labels
plt.text(11.5, 120, '$n$=1')
plt.text(24, 120, '$n$=2')
plt.text(42.5, 120, '$n$=3')
plt.text(58.5, 120, '$n$=4')
plt.text(58.5, 185, '$n$=5')
plt.xlabel('Velocity $v$ [m/s]')
plt.ylabel('Torque $T$ [Nm]')

plt.suptitle('Torque curves for typical car engine');
plt.tight_layout()
plt.savefig("cruise-gearcurves.png", bbox_inches='tight')

PI controller

# Construct a PI controller with rolloff, as a transfer function
Kp = 0.5                        # proportional gain
Ki = 0.1                        # integral gain
control_pi = ct.tf2io(
    ct.TransferFunction([Kp, Ki], [1, 0.01*Ki/Kp]),
    name='control', inputs='u', outputs='y')

cruise_pi = ct.InterconnectedSystem(
    (vehicle, control_pi), name='cruise',
    connections = [('control.u', '-vehicle.v'), ('vehicle.u', 'control.y')],
    inplist = ('control.u', 'vehicle.gear', 'vehicle.theta'), inputs = ('vref', 'gear', 'theta'),
    outlist = ('vehicle.v', 'vehicle.u'), outputs = ('v', 'u'))

Plotting function

# Define a generator for creating a "standard" cruise control plot
def cruise_plot(sys, t, y, t_hill=5, vref=20, antiwindup=False, linetype='b-',
               subplots=[None, None]):
    # Figure out the plot bounds and indices
    v_min = vref-1.2; v_max = vref+0.5; v_ind = sys.find_output('v')
    u_min = 0; u_max = 2 if antiwindup else 1; u_ind = sys.find_output('u')

    # Make sure the upper and lower bounds on v are OK
    while max(y[v_ind]) > v_max: v_max += 1
    while min(y[v_ind]) < v_min: v_min -= 1
        
    # Create arrays for return values
    subplot_axes = subplots.copy()

    # Velocity profile
    if subplot_axes[0] is None:
        subplot_axes[0] = plt.subplot(2, 1, 1)
    else:
        plt.sca(subplots[0])
    plt.plot(t, y[v_ind], linetype)
    plt.plot(t, vref*np.ones(t.shape), 'k-')
    plt.plot([t_hill, t_hill], [v_min, v_max], 'k--')
    plt.axis([0, t[-1], v_min, v_max])
    plt.xlabel('Time $t$ [s]')
    plt.ylabel('Velocity $v$ [m/s]')

    # Commanded input profile
    if subplot_axes[1] is None:
        subplot_axes[1] = plt.subplot(2, 1, 2)
    else:
        plt.sca(subplots[1])
    plt.plot(t, y[u_ind], 'r--' if antiwindup else linetype)
    plt.plot([t_hill, t_hill], [u_min, u_max], 'k--')
    plt.axis([0, t[-1], u_min, u_max])
    plt.xlabel('Time $t$ [s]')
    plt.ylabel('Throttle $u$')

    # Applied input profile
    if antiwindup:
        plt.plot(t, np.clip(y[u_ind], 0, 1), linetype)
        plt.legend(['Commanded', 'Applied'], frameon=False)
        
    return subplot_axes

Trajectory description

# Define the time and input vectors
T = np.linspace(0, 25, 101)
vref = 20 * np.ones(T.shape)
gear = 4 * np.ones(T.shape)
theta0 = np.zeros(T.shape)

# Effect of a hill at t = 5 seconds
theta_hill = np.array([
    0 if t <= 5 else
    4./180. * pi * (t-5) if t <= 6 else
    4./180. * pi for t in T])

Simulated responses (plot)

# Simulate and plot
plt.figure()
plt.suptitle('Response to change in road slope')

subplots = [None, None]
linecolor = ['red', 'blue', 'green']
handles = []
for i, m in enumerate([1200, 1600, 2000]):
    # Compute the equilibrium state for the system
    X0, U0 = ct.find_eqpt(
        cruise_pi, [vref[0], 0], [vref[0], gear[0], theta0[0]], 
        iu=[1, 2], y0=[vref[0], 0], iy=[0], params={'m':m})

    t, y = ct.input_output_response(
        cruise_pi, T, [vref, gear, theta_hill], X0, params={'m':m})

    subplots = cruise_plot(cruise_pi, t, y, t_hill=5, subplots=subplots,
                           linetype=linecolor[i][0] + '-')
    handles.append(mpl.lines.Line2D([], [], color=linecolor[i], 
                   linestyle='-', label="m = %d" % m))

# Add labels to the plots
plt.sca(subplots[0])
plt.ylabel('Speed [m/s]')
plt.legend(handles=handles, frameon=False, loc='lower right');

plt.sca(subplots[1])
plt.ylabel('Throttle')
plt.xlabel('Time [s]');
plt.savefig("cruise-speedresp.png", bbox_inches='tight')

Linearized Dynamics

To explore the behavior of the cruise control system near the equilibrium point we will linearize the system. A Taylor series expansion of the dynamics around the equilibrium point gives

${\frac {d(v-v_{\text{e}})}{dt}}=-a(v-v_{\text{e}})-b_{\text{g}}(\theta -\theta _{\text{e}})+b(u-u_{\text{e}})+{\text{higher-order terms,}}$

where

$a={\frac {\rho C_{\text{d}}A|v_{\text{e}}|-u_{\text{e}}\alpha _{n}^{2}T'(\alpha _{n}v_{\text{e}})}{m}},\qquad b_{\text{g}}=g\cos {\theta _{\text{e}}},\qquad b={\frac {\alpha _{n}T(\alpha _{n}v_{\text{e}})}{m}}.$

Notice that the term corresponding to rolling friction disappears if $v>0$. For a car in fourth gear with $v_{\text{e}}=20$ m/s, $\theta _{\text{e}}=0$, and the numerical values from above, the equilibrium value for the throttle is $u_{\text{e}}=0.1687$ and the parameters are $a=0.01$, $b=1.32$, and $b_{\text{g}}=9.8$. This linear model describes how small perturbations in the velocity about the nominal speed evolve in time.

We apply the PI controller above to the case where the car is running with constant speed on a horizontal road and the system has stabilized so that the vehicle speed and the controller output are constant. The figure to the right shows what happens when the car encounters a hill with a slope of 4 degrees and a hill with a slope of 6 degrees at time $t=\,$ 5 seconds. The results for the nonlinear model are dashed curves and those for the linear model are solid curves. The differences between the curves are very small (especially for $\theta =\,$ 4 degrees), and control design based on the linearized model is thus validated.

Python code

Linearized dynamics

# Find the equilibrium point for the system
Xeq, Ueq = ct.find_eqpt(
    vehicle, [vref[0]], [0, gear[0], theta0[0]], y0=[vref[0]], iu=[1, 2])
print("Xeq = ", Xeq, "\nUeq = ", Ueq)

# Compute the linearized system at the eq pt
vehlin = ct.linearize(vehicle, Xeq, [Ueq[0], gear[0], 0], name='vehlin', copy=True)

PI controller with anti-windup compensation

def pi_update(t, x, u, params={}):
    # Get the controller parameters that we need
    ki = params.get('ki', 0.1)
    kaw = params.get('kaw', 2)  # anti-windup gain

    # Assign variables for inputs and states (for readability)
    v = u[0]                    # current velocity
    vref = u[1]                 # reference velocity
    z = x[0]                    # integrated error

    # Compute the nominal controller output (needed for anti-windup)
    u_a = pi_output(t, x, u, params)

    # Compute anti-windup compensation (scale by ki to account for structure)
    u_aw = kaw/ki * (np.clip(u_a, 0, 1) - u_a) if ki != 0 else 0

    # State is the integrated error, minus anti-windup compensation
    return (vref - v) + u_aw

def pi_output(t, x, u, params={}):
    # Get the controller parameters that we need
    kp = params.get('kp', 0.5)
    ki = params.get('ki', 0.1)

    # Assign variables for inputs and states (for readability)
    v = u[0]                    # current velocity
    vref = u[1]                 # reference velocity
    z = x[0]                    # integrated error

    # PI controller
    return kp * (vref - v) + ki * z

control_pi_aw = ct.NonlinearIOSystem(
    pi_update, pi_output, name='control',
    inputs = ['v', 'vref'], outputs = ['u'], states = ['z'],
    params = {'kp':0.5, 'ki':0.1})

# Create a closed loop controller for the linear system
cruise_lin = ct.InterconnectedSystem(
    (vehlin, control_pi_aw), name='cruise_lin',
    connections=(
        ('vehlin.u', 'control.u'),
        ('control.v', 'vehlin.v')),
    inplist=('control.vref', 'vehlin.gear', 'vehlin.theta'),
    outlist=('control.u', 'vehlin.v'), outputs=['u', 'v'])

# Create a closed loop controller for the nonlinear system
cruise_nonlin = ct.InterconnectedSystem(
    (vehicle, control_pi_aw), name='cruise_nonlin',
    connections=(
        ('vehicle.u', 'control.u'),
        ('control.v', 'vehicle.v')),
    inplist=('control.vref', 'vehicle.gear', 'vehicle.theta'),
    outlist=('control.u', 'vehicle.v'), outputs=['u', 'v'])

Simulations

# Linear response
X0_lin, U0 = ct.find_eqpt(
    cruise_lin, [vref[0], 0], [vref[0], gear[0], theta0[0]],
    y0=[0, vref[0]], iu=[1, 2], iy=[1])

t, y = ct.input_output_response(cruise_lin, T, [vref, gear, theta_hill], X0_lin)
subplots = cruise_plot(cruise_lin, t, y, t_hill=5, linetype='r-')

# Nonlinear response
X0_nonlin, U0 = ct.find_eqpt(
    cruise_nonlin, [vref[0], 0], [vref[0], gear[0], theta0[0]],
    y0=[0, vref[0]], iu=[1, 2], iy=[1])

t, y = ct.input_output_response(cruise_nonlin, T, [vref, gear, theta_hill], X0_nonlin)
subplots = cruise_plot(cruise_nonlin, t, y, t_hill=5, subplots=subplots, linetype='b--') 

# Add a legend to identify linear vs nonlinear
plt.legend(['linear', 'nonlinear'], frameon=False, loc='lower right')

# Add two more simulations for 6 degree hill instead of 4 degree
t, y = ct.input_output_response(cruise_lin, T, [vref, gear, theta_hill*1.5], X0_lin)
subplots = cruise_plot(cruise_lin, t, y, t_hill=5, subplots=subplots, linetype='r-') 

t, y = ct.input_output_response(cruise_nonlin, T, [vref, gear, theta_hill*1.5], X0_nonlin)
subplots = cruise_plot(cruise_nonlin, t, y, t_hill=5, subplots=subplots, linetype='b--') 

# Add titles and legends and save the figure
plt.suptitle('Linear versus nonlinear model response')
plt.sca(subplots[1]); plt.axis([0, 25, 0, 1.2])

plt.savefig("cruise-linear_vs_nonlinear.png", bbox_inches='tight')

State Space Control

The linearized dynamics of the process around an equilibrium point $v_{\text{e}}$, $u_{\text{e}}$ are given by

${\begin{aligned}{\frac {dx}{dt}}&=-ax-b_{\text{g}}\theta +bw,\\y&=v=x+v_{\text{e}},\end{aligned}}$

where $x=v-v_{\text{e}}$, $=u-u_{\text{e}}$, $m$ is the mass of the car, and $\theta$ is the angle of the road. The constants $a$, $b$, and $b_{\text{g}}$ depend on the properties of the car and are given above.

If we augment the system with an integrator, the system dynamics become

${\begin{aligned}{\frac {dx}{dt}}&=-ax-b_{\text{g}}\theta +bw,\\{\frac {dz}{dt}}&=y-v_{\text{r}}=v_{\text{e}}+x-v_{\text{r}},\end{aligned}}$

or, in state space form,

${\frac {d}{dt}}{\begin{bmatrix}x\\z\end{bmatrix}}={\begin{bmatrix}-a&0\\1&0\end{bmatrix}}{\begin{bmatrix}x\\z\end{bmatrix}}+{\begin{bmatrix}b\\0\end{bmatrix}}w+{\begin{bmatrix}-b_{\text{g}}\\0\end{bmatrix}}\theta +{\begin{bmatrix}0\\v_{\text{e}}-v_{\text{r}}\end{bmatrix}}.$

Note that when the system is at equilibrium, we have that ${\dot {z}}=0$, which implies that the vehicle speed $v=v_{\text{e}}+x$ should be equal to the desired reference speed $v_{\text{r}}$. Our controller will be of the form

${\begin{aligned}{\frac {dz}{dt}}&=y-v_{\text{r}},\\w&=-k_{\text{p}}x-k_{\text{i}}z+k_{\text{f}}v_{\text{r}},\end{aligned}}$

and the gains $k_{\text{p}}$, $k_{\text{i}}$, and $k_{\text{f}}$ will be chosen to stabilize the system and provide the correct input for the reference speed.

Assume that we wish to design the closed loop system to have the characteristic polynomial

$\lambda (s)=s^{2}+a_{1}s+a_{2}.$

Setting the disturbance $\theta =0$, the characteristic polynomial of the closed loop system is given by

$\det {\bigl (}sI-(A-BK){\bigr )}=s^{2}+(bk_{\text{p}}+a)s+bk_{\text{i}},$

and hence we set

$k_{\text{p}}={\frac {a_{1}-a}{b}},\qquad k_{\text{i}}={\frac {a_{2}}{b}},\qquad k_{\text{f}}={-1}/{\bigl (}C(A-BK)^{-1}B{\bigr )}={\frac {a_{1}}{b}}.$

The resulting controller stabilizes the system and hence brings ${\dot {z}}=y-v_{\text{r}}$ to zero, resulting in perfect tracking. Notice that even if we have a small error in the values of the parameters defining the system, as long as the closed loop eigenvalues are still stable, then the tracking error will approach zero. Thus the exact calibration required in our previous approach (using $k_{\text{f}}$) is not needed here. Indeed, we can even choose $k_{\text{f}}=0$ and let the feedback controller do all of the work. However, $k_{\text{f}}$ does influence the transient response to reference signals and setting it properly will generally give a more favorable response.

Integral feedback can also be used to compensate for constant disturbances. The figure to the right shows the results of a simulation in which the car encounters a hill with angle $\theta =4$ degrees at $t=$ 5 seconds. The steady-state values of the throttle for a state feedback controller and a controller with integral action are very close, but the corresponding values of the car velocity are quite different. The reason for this is that the zero frequency gain from throttle to velocity is $-b/a=130$ is high. The stability of the system is not affected by this external disturbance, and so we once again see that the car's velocity converges to the reference speed. This ability to handle constant disturbances is a general property of controllers with integral feedback.

Python code

State feedback controller

def sf_update(t, z, u, params={}):
    y, r = u[1], u[2]
    return y - r

def sf_output(t, z, u, params={}):
    # Get the controller parameters that we need
    K = params.get('K', 0)
    ki = params.get('ki', 0)
    kf = params.get('kf', 0)
    xd = params.get('xd', 0)
    yd = params.get('yd', 0)
    ud = params.get('ud', 0)

    # Get the system state and reference input
    x, y, r = u[0], u[1], u[2]

    return ud - K * (x - xd) - ki * z + kf * (r - yd)

# Create the input/output system for the controller
control_sf = ct.NonlinearIOSystem(
    sf_update, sf_output, name='control',
    inputs=('x', 'y', 'r'),
    outputs=('u'),
    states=('z'))

# Create the closed loop system for the state space controller
cruise_sf = ct.InterconnectedSystem(
    (vehicle, control_sf), name='cruise',
    connections=(
        ('vehicle.u', 'control.u'),
        ('control.x', 'vehicle.v'),
        ('control.y', 'vehicle.v')),
    inplist=('control.r', 'vehicle.gear', 'vehicle.theta'),
    outlist=('control.u', 'vehicle.v'), outputs=['u', 'v'])
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Simulation (plot)
# Define the time and input vectors
T = np.linspace(0, 25, 501)
vref = 20 * np.ones(T.shape)
gear = 4 * np.ones(T.shape)
theta0 = np.zeros(T.shape)

# Find the equilibrium point for the system
Xeq, Ueq = ct.find_eqpt(
    vehicle, [vref[0]], [0, gear[0], theta0[0]], y0=[vref[0]], iu=[1, 2])
print("Xeq = ", Xeq)
print("Ueq = ", Ueq)

# Compute the linearized system at the eq pt
cruise_linearized = ct.linearize(vehicle, Xeq, [Ueq[0], gear[0], 0])
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Further Reading
* How Stuff Works: cruise control
* Wikipedia: cruise control