k is the spring constant of the spring. x is the distance the spring is compressed. M is the mass of the box. θ (theta) is the angle of the ramp from the horizontal. h is the maximum height reached by the box. The scenario is repeated with the box compressing the spring a distance that is larger than the original distance x. (b) Students derive an equation for the maximum height h in the original scenario, h=(sin2θ)kx22Mg, which may or may not be correct. Is this equation consistent with your claim in part (a)? Explain why or why not.

College Physics
10th Edition
ISBN:9781285737027
Author:Raymond A. Serway, Chris Vuille
Publisher:Raymond A. Serway, Chris Vuille
Chapter1: Introduction
Section: Chapter Questions
Problem 45P: In Figure P1.49, find (a) the side opposite , (b) the side adjacent to . (c) cos , (d) sin , and (c)...
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A box is pressed against a horizontal spring, compressing the spring from its relaxed length. The box is then released and the spring launches the box horizontally along a track that ends in a ramp, as shown above. The box has enough speed to leave the ramp, and the box reaches a maximum vertical height above the floor. Assume there is negligible friction between the box and the track and air resistance is negligible.

  • k is the spring constant of the spring.
  • x is the distance the spring is compressed.
  • M is the mass of the box.
  • θ (theta) is the angle of the ramp from the horizontal.
  • h is the maximum height reached by the box.
  • The scenario is repeated with the box compressing the spring a distance that is larger than the original distance x.

    (b) Students derive an equation for the maximum height h in the original scenario, h=(sin2θ)kx22Mg, which may or may not be correct. Is this equation consistent with your claim in part (a)? Explain why or why not.

k
0000000. M
Transcribed Image Text:k 0000000. M
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