Moving on to 3D
Suppose our bike goes around in a circle rather than in a line.
We want to be able to parametrize a reflector's motion. Looking from
above, suppose
- the bike turns in a circle of radius 20 feet in a
counterclockwise direction;
- we let z=0 be the plane of the road;
- the reflector is 1 foot from the center of the wheel.
We can try to parametrize using the same strategy of breaking the
motion into components.
Question #5
- Let c(t) be the motion of the center of the wheel traveling
in around the 20 foot circle. Parametrize c(t) as a three-dimensional curve.
- Find a function g(t) the describes the motion of the reflector
relative to the wheel's center.
Here are some hints:
- At time t, the bicycle tire forms the plane
spanned by the vertical direction and by a
tangent vector to the 20 foot circle.
- Determine the vertical component of the reflector by arguing that
it has the form (0,0,A sin(wt)) where
A and w are constants determined by the
size and speed of the bicycle.
- If T(t) is the unit tangent vector to the large circle
at time t, then argue that the horizontal component of motion
has the magnitude A cos(wt) and is in the
direction of T(t).
- The motion of the reflector is therefore given parametrically by
c(t)+g(t). Write down this expression and check your answer
by using the
ParamPlot3D
or spacecurve
command.
An example of the
syntax for ParamPlot3D
is
ParamPlot3D([2*cos(t), 2*sin(t), 5*sin(t)], t=0..2*Pi);
Question #6
If we let t vary from 0 infinity, will the
reflector trace out a closed curve? If the curve is not closed, can
the reflector be moved to a positive distance from the wheel's center
to make it a closed loop? If the curve is already closed, can you
move the reflector to make a curve that never closes?
Next: Tying the Knot
Up: Introduction
Previous: It's Like Riding a Bicycle
Frederick J. Wicklin <fjw@geom.umn.edu>
Jeremy Case
Document Created: Mon Feb 20
Last modified: Tue Feb 27 08:51:53 1996