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Can the diver of Fig. 8–28 do a somersault without having any initial rotation when she leaves the board? Explain.

Short Answer

Expert verified

Yes, the diver can perform a somersault without having any initial rotation when she leaves the board.

Step by step solution

01

Calculation of angular acceleration 

The angular acceleration of an object can be calculated by dividing the value of the torque by the MOI of the object.

Its value is altered inversely to the value of the MOI of the object.

02

Conservation of angular momentum

The diver can perform a somersault without having any initial rotation when she leaves the board. This is because to perform a somersault, the diver requires some initial angular momentum.

According to the law of conservation of angular momentum, when a body is expanded, the moment of inertia is higher; and hence the angular velocity is shorter.

Moreover, when arms and legs are tucked during the somersault, the moment of inertia is smaller; therefore, the angular velocity rises. When she pushes the board while leaving it, it provides her an initial angular momentum about her center of mass.

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Most popular questions from this chapter

Two blocks, each of mass m, are attached to the ends of a massless rod which pivots as shown in Fig. 8–43. Initially the rod is held in the horizontal position and then released. Calculate the magnitude and direction of the net torque on this system when it is first released.

An Atwood machineconsists of two masses,\({m_A} = {\bf{65 kg}}\) and\({m_B} = {\bf{75 kg}}\) connected by a massless inelastic cord that passes over a pulley free to rotate, Fig. 8 52. The pulley is a solid cylinder of radius\(R = {\bf{0}}{\bf{.45 m}}\) and mass 6.0 kg. (a) Determine the acceleration of each mass. (b) What % error would be made if the moment of inertia of the pulley is ignored? (Hint: The tensions\({F_{TA}}\) and\({F_{TB}}\)are not equal. We discussed the Atwood machine in Example 4–13, assuming I = 0 for the pulley.)

FIGURE 8-52 Problem 47.Atwood machine.

An automobile engine slows down from 3500 rpm to 1200 rpm in 2.5 s. Calculate (a) its angular acceleration, assumed constant, and (b) the total number of revolutions the engine makes in this time.

Two wheels having the same radius and mass rotate at the same angular velocity (Fig. 8–38). One wheel is made with spokes so nearly all the mass is at the rim. The other is a solid disk. How do their rotational kinetic energies compare?

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(b) The wheel with spokes has about twice the KE.

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FIGURE 8-38

MisConceptual Question 7.

On a 12.0-cm-diameter audio compact disc (CD), digital bits of information are encoded sequentially along an outward spiraling path. The spiral starts at radius \({{\bf{R}}_{\bf{1}}}{\bf{ = 2}}{\bf{.5}}\;{\bf{cm}}\) and winds its way out to radius \({{\bf{R}}_{\bf{2}}}{\bf{ = 5}}{\bf{.8}}\;{\bf{cm}}\). To read the digital information, a CD player rotates the CD so that the player’s readout laser scans along the spiral’s sequence of bits at a constant linear speed of 1.25 m/s. Thus the player must accurately adjust the rotational frequency f of the CD as the laser moves outward. Determine the values for f (in units of rpm) when the laser is located at \({{\bf{R}}_{\bf{1}}}\) and when it is at \({{\bf{R}}_{\bf{2}}}\).

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