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A uniform, solid, \( 100 \) \( \text{kg} \) cylinder with a diameter of \( 1.0 \) \( \text{m} \) is mounted so it is free to rotate about a fixed, horizontal, frictionless axis that passes through the centers of its circular ends. A \( 10 \) \( \text{kg} \) block is hung from a very light, thin cord wrapped around the cylinder’s circumference. When the block is released, the cord unwinds and the block accelerates downward, as shown in the figure. What is the acceleration of the block?

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A man with mass \( m \) is standing on a rotating platform in a science museum. The platform can be approximated as a uniform disk of radius \( R \) that rotates without friction at a constant angular velocity \( \omega \). The surface of the platform is frictionless, so the only forces between the man and the platform arise from the man’s feet as he runs. Two students are discussing what the man should do if he wishes to remain directly above a single point on the platform’s surface (so that, as viewed from the ground, he does not drift relative to that point).Student A claims that the man should run clockwise, in the same direction that the platform is rotating, because doing so will decrease the system’s moment of inertia and therefore increase \( \omega \), allowing him to stay above the desired point.Student B claims that, because no external torque acts on the man–platform system, the man must instead run counter-clockwise (opposite the platform’s rotation) so that the total angular momentum of the system about its central axis is conserved.Briefly explain which student’s reasoning is correct, explicitly referring to conservation of angular momentum and the absence (or presence) of external torques.

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Two masses, \( m_1 \) and \( m_2 \), are suspended on either side of a pulley with a radius \( R \), as shown. The heavier mass, \( m_2 \), is initially held at rest above the ground by a distance \( h \) before being released. An experimenting elephant measures that it takes an amount of time \( t \) for the heavier mass to hit the ground after being released.\n(a) The pulley is an odd shape, and the elephant would like to measure its moment of inertia. Derive an algebraic expression for the moment of inertia of the pulley in terms of only quantities measured or known by the elephant (\( m_1, m_2, R, h, t \) and physical constants).\n(b) How many radians has the pulley rotated from the time it was released to the time \( m_2 \) hit the ground? Express your answer in terms of \( m_1, m_2, R, h \) and physical constants.

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An \( 80 \, \text{kg} \) block is placed \( 2 \, \text{m} \) away from the endpoint of a horizontal steel beam of length \( 6.6 \, \text{m} \) and mass \( 1,450 \, \text{kg} \). The plank makes contact with a vertical wall on one end, and the other endpoint is attached to a massless cable that makes an angle of \( 30^\circ \) with the horizontal and ties into the vertical wall as well. Calculate the magnitude and direction of the force between the cable and the wall and of the force between the steel beam and the wall.

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A uniform ladder with mass \( m_2 \) and length \( L \) rests against a smooth wall. A do-it-yourself enthusiast of mass \( m_1 \) stands on the ladder a distance \( d \) from the bottom (measured along the ladder). The ladder makes an angle \( \theta \) with the ground. There is no friction between the wall and the ladder, but there is a frictional force of magnitude \( f \) between the floor and the ladder.\( N_1 \) is the magnitude of the normal force exerted by the wall on the ladder, and \( N_2 \) is the magnitude of the normal force exerted by the ground on the ladder. Throughout the problem, consider counterclockwise torques to be positive.

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