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Three disks are spinning independently on the same axle without friction. Their respective rotational inertias and angular speeds are I,ω𝐼,𝜔 (clockwise); 2I,3ω2𝐼,3𝜔 (counterclockwise); and 4I,ω/24𝐼,𝜔/2 (clockwise). The disks then slide together and stick together, forming one piece with a single angular velocity. What will be the direction and the rate of rotation ωnet𝜔net of the single piece?Express your answer in terms of one or both of the variables I𝐼 and ω𝜔 and appropriate constants. Use a minus sign for clockwise rotation.View Available Hint(s)for Part HActivate to select the appropriates template from the following choices. Operate up and down arrow for selection and press enter to choose the input value typeActivate to select the appropriates symbol from the following choices. Operate up and down arrow for selection and press enter to choose the input value typeωnet𝜔net =

Question

Three disks are spinning independently on the same axle without friction. Their respective rotational inertias and angular speeds are I,ω𝐼,𝜔 (clockwise); 2I,3ω2𝐼,3𝜔 (counterclockwise); and 4I,ω/24𝐼,𝜔/2 (clockwise). The disks then slide together and stick together, forming one piece with a single angular velocity. What will be the direction and the rate of rotation ωnet𝜔net of the single piece?Express your answer in terms of one or both of the variables I𝐼 and ω𝜔 and appropriate constants. Use a minus sign for clockwise rotation.View Available Hint(s)for Part HActivate to select the appropriates template from the following choices. Operate up and down arrow for selection and press enter to choose the input value typeActivate to select the appropriates symbol from the following choices. Operate up and down arrow for selection and press enter to choose the input value typeωnet𝜔net =

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Solution 1

The conservation of angular momentum states that the total angular momentum before the disks stick together is equal to the total angular momentum after they stick together.

Before they stick together, the total angular momentum is the sum of the angular momenta of the three disks. The angular momentum of a rotating object is given by the product of its rotational inertia and its angular speed.

For the first disk, the angular momentum is Iω (clockwise, so we'll consider it as negative). For the second disk, the angular momentum is 2I3ω (counterclockwise, so it's positive). For the third disk, the angular momentum is 4I*(ω/2) (clockwise, so it's negative).

So, the total angular momentum before they stick together is -Iω + 6Iω - 2Iω = 3Iω.

After they stick together, the total rotational inertia is the sum of the rotational inertias of the three disks, which is I + 2I + 4I = 7I.

Let's denote the final angular velocity as ωnet. According to the conservation of angular momentum, we have:

7I * ωnet = 3Iω.

Solving for ωnet, we get:

ωnet = 3Iω / 7I = 3ω / 7.

Since the result is positive, the final rotation is counterclockwise.

This problem has been solved

Solution 2

The conservation of angular momentum states that the total angular momentum before the disks stick together is equal to the total angular momentum after they stick together.

Before they stick together, the total angular momentum is the sum of the angular momenta of the three disks. The angular momentum of a rotating object is given by the product of its rotational inertia and its angular speed.

For the first disk, the angular momentum is Iω (clockwise, so we'll consider it as negative). For the second disk, the angular momentum is 2I(-3ω) (counterclockwise, so it's positive). For the third disk, the angular momentum is 4I*ω (clockwise, so it's negative).

So, the total angular momentum before they stick together is -Iω + 2I3ω - 4Iω/2 = 6Iω - 2Iω = 4Iω.

After they stick together, the total angular momentum is the product of the total rotational inertia and the angular speed of the single piece. The total rotational inertia is the sum of the rotational inertias of the three disks, which is I + 2I + 4I = 7I.

So, the total angular momentum after they stick together is 7I*ωnet.

Setting these two equal gives 4Iω = 7I*ωnet.

Solving for ωnet gives ωnet = 4ω/7.

Since the result is positive, the direction of rotation is counterclockwise.

So, the single piece will rotate at a rate of 4ω/7 in the counterclockwise direction.

This problem has been solved

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