Angular momentum of merry go round turntable

In summary, the question is asking for the angular velocity of a turntable after a person begins running on it, and the solution involves using conservation of angular momentum. The person is treated as a point mass with moment of inertia mr^2.
  • #1
MAins
18
0
Hi, I got this question wrong on a test and am really quite lost about it. I'd appreciate somebody running me through it.

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"Suppose a 55 kg person stands at the edge of a 6.5 m diameter merry go round turntable that is mounted on a frictionless bearing and has a moment of inertia of 1700 kg m^2. The turntable is at rest initially, but when the person begins running at a speed of 3.8 m/s (with respect to the turntable) around its edge, the turntable begins to rotate in the opposite direction. Caculate the angular velocity of the table."

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So I set up conservation of angular momentum
L_f = L_i
and
(Iw)_f = (Iw)_i

Can somebody please help me from there?
 
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  • #2
I guess you'd treat the person as a point mass, so the person has moment of inertia mr^2. Can you calculate his angular velocity?
 
  • #3


Hi, it seems like you are on the right track with using conservation of angular momentum and the equation (Iw)_f = (Iw)_i. Let's break down the problem step by step to find the solution.

First, let's define our variables:
m = mass of person (55 kg)
r = radius of merry go round (6.5 m)
I = moment of inertia of the turntable (1700 kg m^2)
w = angular velocity of the turntable (unknown)
v = linear velocity of the person (3.8 m/s)

Next, let's consider the initial and final states of the system. Initially, the turntable is at rest and the person is running at a speed of 3.8 m/s around its edge. This means that the person has a linear velocity of 3.8 m/s with respect to the turntable, but they are also rotating with the turntable at the same angular velocity. So we can say that the initial angular velocity of the turntable is also 3.8 m/s.

Now, let's use the equation (Iw)_f = (Iw)_i to find the final angular velocity (w) of the turntable. Plugging in our values, we get:
(1700 kg m^2)(w) = (55 kg)(6.5 m)(3.8 m/s)
Solving for w, we get:
w = (55 kg)(6.5 m)(3.8 m/s) / (1700 kg m^2)
w = 0.75 rad/s

Therefore, the angular velocity of the turntable is 0.75 rad/s in the opposite direction of the person's motion. This means that the turntable is rotating at a slower speed than the person is running, but in the opposite direction.

I hope this explanation helps you understand the problem better. Remember to always define your variables and consider the initial and final states of the system when solving problems involving conservation of angular momentum. Best of luck in your studies!
 

FAQ: Angular momentum of merry go round turntable

What is angular momentum?

Angular momentum is a measure of an object's rotational motion, taking into account both its mass and its velocity.

How is angular momentum related to the merry go round turntable?

The merry go round turntable has angular momentum because it is rotating around a fixed axis. The amount of angular momentum it has depends on the mass of the turntable and how fast it is rotating.

What factors affect the angular momentum of the merry go round turntable?

The two main factors that affect the angular momentum of the merry go round turntable are its mass and its rotational speed. The greater the mass and the faster the speed, the greater the angular momentum.

What happens to the angular momentum of the turntable if the rotational speed increases?

If the rotational speed of the turntable increases, its angular momentum will also increase. This is because the rotational speed is directly proportional to the angular momentum.

How is angular momentum conserved in a system involving the merry go round turntable?

According to the law of conservation of angular momentum, the total angular momentum in a closed system remains constant. This means that any changes in the angular momentum of the turntable will be balanced out by changes in the angular momentum of other objects in the system, such as riders or additional turntables.

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