A merry -go-round rotates at the rate of 0.4rev / s with an 78 kg man standing at a point 1.5 m from the axis of rotation. What is the new angular speed when the man walks to a point m from the center? Consider the merry-go-round is a solid 11 kg cylinder of radius of 1,5 m. Answer in units of rad/s. 024 (part 2 of 2) 10.0 points What is the change in kinetic energy due to this movement ? Answer in units of

Answers

Answer 1
Answer:

1) Final angular velocity is 5.22 rad/s

2) Change in kinetic energy: 639.8 J

Explanation:

1)

In absence of external forces, the angular momentum of the merry-go-round must be conserved.

So we can write:

L_1 = L_2\nI_1\omega_1 = I_2 \omega_2

where

I_1 is the initial moment of inertia

I_2 is the final moment of inertia

\omega_1 is the initial angular velocity

\omega_2 is the final angular velocity

At the beginning, we have:

\omega_1=0.4 rev/s \cdot 2\pi = 2.51 rad/s

The moment of inertia is the sum of the moment of inertia of the cylinder + the moment of inertia of the man, therefore:

I_1 = (1)/(2)MR^2+mr^2=(1)/(2)(11)(1.5)^2+(78)(1.5)^2=187.9 kgm^2

The man later walks to a point 1 m from the centre, so the final moment of inertia is:

I_2 = (1)/(2)MR^2+mr^2=(1)/(2)(11)(1.5)^2+(78)(1)^2=90.4 kgm^2

Therefore, the final angular velocity is

\omega_2 = (I_1 \omega_1)/(I_2)=((187.9)(2.51))/(90.4)=5.22 rad/s

2)

The angular velocity of the merry-go-round rotating is given by

K=(1)/(2)I\omega^2

In the  first situation, we have

I_1 = 187.9 kg m^2\n\omega=2.51 rad/s

Therefore

K_1 = (1)/(2)(187.9)(2.51)^2=591.8 J

In the second situation, we have

I_2= 90.4 kg m^2\n\omega_2=5.22 rad/s

Therefore

K_2=(1)/(2)(90.4)(5.22)^2=1231.6 J

So the change in kinetic energy is

\Delta K = K_2 - K_1 = 1231.6-591.8=639.8 J

Learn more about circular motion:

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