ch06-p059

# ch06-p059 - 59 The free-body diagram for the ball is shown...

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Unformatted text preview: 59. The free-body diagram for the ball is shown below. Tu is the tension exerted by the upper string on the ball, T is the tension force of the lower string, and m is the mass of the ball. Note that the tension in the upper string is greater than the tension in the lower string. It must balance the downward pull of gravity and the force of the lower string. (a) We take the +x direction to be leftward (toward the center of the circular orbit) and +y upward. Since the magnitude of the acceleration is a = v2/R, the x component of Newton’s second law is mv 2 Tu cosθ + T cosθ = , R where v is the speed of the ball and R is the radius of its orbit. The y component is Tu sin θ − T sin θ − mg = 0. The second equation gives the tension in the lower string: T = Tu − mg / sin θ . Since the triangle is equilateral θ = 30.0°. Thus T = 35.0 N − (b) The net force has magnitude Fnet,str = (Tu + T ) cos θ = (35.0 N + 8.74 N) cos 30.0° = 37.9 N. (1.34 kg)(9.80 m/s 2 ) = 8.74 N. sin 30.0° (c) The radius of the path is R = ((1.70 m)/2)tan 30.0° = 1.47 m. Using Fnet,str = mv2/R, we find that the speed of the ball is v= RFn et,str m = (1.47 m)(37.9 N) = 6.45 m/s. 1.34 kg (d) The direction of Fn et,str is leftward (“radially inward’’). ...
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## This note was uploaded on 05/17/2011 for the course PHY 2049 taught by Professor Any during the Spring '08 term at University of Florida.

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