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Circular Motion Lab
“An object that moves in a circle at constant speed v is said to undergo uniform circular motion. Examples are a ball on the end of a string revolved around one’s head.” –Douglas Giancoli
Purpose This lab will allow us to examine the relationship between
mass, Theory 1. (The Law of Inertia) 2. (acceleration = Fnet/mass) The acceleration of an object produced by the sum of all forces acting on the object (the net force) is directly proportional to the magnitude of the net force, in the same direction as the net force, and inversely proportional to the mass of the object. 3. For every action, there is an equal and opposite reaction. When a mass on a string swings steadily around in a circle we call it uniform circular motion. They speed is constant, but since the direction is continually changing, the velocity vector (the direction is changing) and a constant acceleration. Even though the speed is constant, the velocity (speed and direction) is constantly changing and so the acceleration is not zero. Since the velocity of the mass is always changing direction toward the center of the circle. It follows then that the mass is always accelerating toward the center of the circle. That “center-seeking”, radial, or centripetal acceleration (aR) is given by the following expression:
Your teacher will now prove this for you, so listen carefully, take good notes and ask questions about what you would like explained more better. Newton’s second law is encapsulated in the formula acceleration = (net force)/mass or
The arrows are used to indicate that the force and the acceleration are vectors. It is assumed that the mass is constant (this is crucial for the formula to work.)
So if you know the centripetal acceleration Materials (or improvise similar) · A piece of string, 1 to 1.5 meters long · Several washers or nuts to use as weights · Masking tape · Meter stick · Timer
Procedure ·
This lab
requires you to swing masses on the end of a string with uniform circular
motion to examine what happens as you change three quantities: the mass, the
length of the string, and the velocity. That is, what happens to the centripetal
force when you change v, r,
and m?
It makes sense to divide this lab into three parts that will examine each of
these. ·
To get
started, tie a knot at the end of your string that will act as a stop. It is important
to make a good stop so that your masses do not fly off when you start
swinging your string. We don’t want anyone getting hurt. ·
To
calculate velocity, use your timer and the equation for the circumference of
a circle (2πr).
Note that to measure velocity you can approximate the time of one revolution
as the average time of 10-20 revolutions. ·
A table is
provided to help you organize your data. In the column labeled “Feel” of the Force,
you will enter words like “greater, less, same.” You will put a word there that
describes how the force of the rope in your hand feels compared to the
initial force. Do an initial trial first to have a baseline, and then for
each trial record whether the force is less, greater, or the same. · You may work through the three parts of this lab in any order you wish.
Part 1: How Mass Affects FC
Part 2: How Velocity Affects FC
Part 3: How Radius Affects FC
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Part 1 |
Mass |
Velocity |
Radius |
“Feel” of the force |
Calculated |
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Initial |
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X |
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Trial #1 |
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Trial #2 |
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Trial #3 |
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Part 2 |
Mass |
Velocity |
Radius |
“Feel” of the force |
Calculated |
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Initial |
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X |
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Trial #1 |
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Trial #2 |
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Trial #3 |
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Part 3 |
Mass |
Velocity |
Radius |
“Feel” of the force |
Calculated |
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Initial |
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X |
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Trial #1 |
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Trial #2 |
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Trial #3 |
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