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Cart on Frictionless Inclined Plane

Galileo used motion on an inclined plane to learn about the free fall. For us it is mainly an exercise to illustrate the properties of the normal and gravitational force and to learn how to work with Newtons laws as vector equations.

We will set ourselves the task of determining what the final velocity of the vehicle will be at the end of the incline.

Because we are interested in the motion of the vehicle we choose to apply Newtons laws to it only. The forces acting on it are

  1. Force of gravity tex2html_wrap_inline164 with magnitude mg
  2. Normal force from surface of incline tex2html_wrap_inline168
Because of the incline these two forces are not parallel and hence gravity and normal force cannot cancel each other out. This means that there will be a net force acting on the vehicle and it will therefore necessarily undergo motion with constant acceleration. To figure the acceleration we need to obtain an expression for the net force. For this purpose it is convenient to deal with one component of force at a time. We choose the directions to be considered such that coordinate system such that
one of the directions of the coordinate system will be parallel to the net force.
Other choices are not wrong but give less elegant solutions to the problem.

Because we expect the net force to be parallel to the incline we choose the tex2html_wrap_inline170 vector parallel to the incline. The two components of the net force are
eqnarray14
where tex2html_wrap_inline172 is the angle of the incline. If the brick does not sink into the plane then
eqnarray18
This implies that
equation21
From Newton's second law this implies that the vehicle moves with constant acceleration:
eqnarray26
Now I use my knowledge of kinematics to figure the final velocity. Remember the handy equationwhich leaves the time taken for the motion out:
equation33
Where d denotes the length of the inclined surface Lets say we start from rest at the top of the incline, then the final velocity will be
eqnarray35

But we recognize tex2html_wrap_inline176 as the height, h, of the incline so finally we get
equation37
Amusingly this is exactly the velocity after a free fall over the distance h. The length of the incline does not affect the final velocity only the time it takes to get to the end!

To test our formulae we use our beloved air-track. We have set up the photo-gate to measure the time taken for the vehicle to pass it. This time is related to the velocity by
equation40
where tex2html_wrap_inline182 is the length of the vehicle. For this time we predict
equation44
We put in numbers to get
equation48
We do the experiment and get a number indistinguishable from this.


next up previous
Next: Tension in a String: Up: Illustrative Applications of Newtons Previous: Illustrative Applications of Newtons

Collin Broholm
Tue Sep 23 23:16:07 EDT 1997