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
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
vector parallel to the incline. The two components
of the net force are
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where
is the angle of the incline. If the brick does not
sink into the plane then
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This implies that
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From Newton's second law this implies that the vehicle moves with constant
acceleration:

Now I use my knowledge of kinematics to figure the final velocity. Remember the
handy equationwhich leaves the time taken for the motion out:
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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
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But we recognize
as the height, h, of the incline so finally we get
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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
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where
is the length of the vehicle. For this time we predict
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We put in numbers to get

We do the experiment and get a number indistinguishable from this.