# Bungee Jumping

*This exercise requires the solution of linear second order
equations. Maximum and minimum values of *
*parameters**
must be found to allow a person to survive a jump. The meaning of
**zeros
of the solution** and its derivative, as well as the
effect of a **nonlinear term**, are discussed
qualitatively. *

Suppose that you are a bungee jumper, standing on a bridge somewhere in Colorado. Three hundred feet below you, a lovely little stream meanders through a scenic canyon. The lovely stream is six inches deep, and has lots of sharp pointy rocks in it. You have brought a variety of cords with which to secure your feet, ranging in stiffness from a steel cable to a soft rubber band. Every one of the cords is exactly 160 feet long, when hung from the bridge. If you choose a cord that is too stiff, then your body will no longer form a connected set after you hit the end of the cord. On the other hand, if you choose one that is too soft, your body may still be moving for a short time after you pass the point 300 feet below where you are standing. Which cord should you choose, if any?

This physical system was studied by famous bungee jumper Robert Hooke about 300 years ago. Hooke's Law states that the force exerted on your body by the cord is proportional to the distance of your body past the equilibrium position of the spring. For the present, we will consider all of the mass of your body to be in your feet (the very fact that you are jumping indicates that your head is not very massive). When your body is above the equilibrium position of the cord, then the cord bends, so you may assume that it exerts no force on your body. On the other hand, the force of gravity acts relentlessly on your body. Finally, there is a certain amount of frictional force applied by air resistance. Assume that it is proportional to velocity, and opposes whatever motion is taking place.

The action of these forces may be summarized as follows. Let *x*
= *x*(*t*) denote the distance of your body from the
end of the bungee cord, i.e. from an imaginary point 160 feet
below the bridge. Let the bridge be at *x*=-160 feet, and
the creek be at *x*=140 feet. Thus *x* increases as you
fall. Define

where *k* is a constant describing the stiffness of the
cord. The larger *k* becomes, the less stretch there is in
the cord. The frictional force has the form . Thus the forces may be summed as

**Problem 1:** Convert this to
a first
order system of equations.

Now, you can see that when you come to rest after the jump, your feet will be more than 160 feet below the bridge. After all, gravity is pulling you downward, while the spring exerts no upward force until your feet are more than 160 feet below the bridge.

**Problem 2:** Find the
distance below the bridge that your feet find themselves when you
come to rest after the jump for any given cord with stiffness *k*.
Use the knowledge that you are six feet tall and weigh 160 lbs.,
and the fact that you do not want to rest below the level of the
creek, to specify a lower bound on the value for *k* that
you require for your bungee cord. Use . Click here to receive the
*DynaSys* Bungee data file for this problem.

Of course, the simple knowledge that your final rest position lies above the level of the stream may not comfort you that greatly. What you really want to know is how far below the bridge you will fall on your first bounce. After that, the frictional force should take over, and each subsequent bounce should not take you so close to the stream bed. The plot below will allow you to plot your position versus your velocity if air resistance is neglected.

**Problem 3:**** **Use the
applet and the *k* value you found in problem 2
to estimate how far you would fall if there were no air.

**Problem 4:** Solve the differential
equation in the case that *a=0*. You need only to
solve from time *t=0* until the first time that . Denote this time . When the velocity is zero, that indicates that your
body is changing direction, and will go up for a while. Compute
the minimum value of the spring
coefficient *k *that will permit you to survive your
jump.

**Problem 5:** When there is
no damping of the motion (air resistance), then your trip back
upwards after bottoming out will be exactly the opposite of the
trip down. Use this fact and the set of axes below to make three
plots of the solution curve you have found: one in the *(t,x)
*plane, one in the plane, and one in the phase plane . Interpret the significance of the intercepts
of the curve in the phase plane.

If there were no damping, you would keep bouncing on the end
of your cord forever. Fortunately for you, there is air
resistance to slow you down. We have already included a linear
term for air resistance in the equation above. Such a linear
term is unrealistic as a model for air resistance, but we
will use it anyway, for the moment. The coefficient is *a~1*,
neglecting such factors as body orientation, clothing, and so on.
Since the equation is still linear, you may still solve it.

**Problem 6:** Solve the differential
equation in the case that *a=.2*. Recompute the
minimum value of *k* that will allow the cord to stop your
fall before unpleasant things happen. Test your answer by
plotting the solution below.

Let us use a more realistic term for the air resistance. The air resistance is actually a nonlinear function of speed. For this reason, we rewrite the equation as

You will probably not be able to calculate a closed-form
solution for this last equation. Instead, use the plot below
to compute the solution to the linear equation and that of
the nonlinear equation on the same plot. The phase plane appears
on the left, a plot of the distance versus time appears at top
right, and velocity versus time appears at bottom right. Use a
value for of .005. Click
here to receive the
*DynaSys* Bungee data file for this problem.

**
Problem 7:** Compare qualitatively the solutions
for linear air resistance and for nonlinear resistance.

As was mentioned earlier, it is possible for a cord to be too stiff. For example, if you were to jump from the bridge attached to a steel cable, then being stopped by the cable would probably not be significantly better than being stopped by the ground. Suppose we know that a human body tied to a rope can only withstand a pull, from the rope, of about twenty times its weight, beyond which force being caught by the rope is about as bad as hitting the ground.

**Problem 8:** Use this
hypothesis to compute the maximum allowable value for *k*
for a good bungee cord.

**Problem 9:**Use a computer
to draw phase portraits for four of your cords: a
collection of rubber bands tied together with *k=.2*, a
bungee cord with *k=6,* a climbing rope with *k=10*,
and a steel cable with *k=300*. Which of these is safe?
Interpret each plot.

**Problem 10:** Explain why
there are no bungee cords that permit your body to come smoothly
to a halt, i.e. you always bounce on the end of the cord.

With the advent of HTML5, Javascript is now ready for prime time
for mathematical applications. There are
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help students learn Calculus.