Ch 10: Interactions and Potential Energy
Chapter 10, Problem 10
CALC A clever engineer designs a 'sprong' that obeys the force law Fx=−q(x−xeq)³ , where xeq is the equilibrium position of the end of the sprong and q is the sprong constant. For simplicity, we'll let xeq=0 m .Then Fx=−qx³. b. Find an expression for the potential energy of a stretched or compressed sprong.
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Textbook Question
A system has potential energy U(x)=(10 J)[1−sin((3.14 rad/m) x)] as a particle moves over the range 0 m≤x≤3 m
b. For each, is it a point of stable or unstable equilibrium?
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Textbook Question
CALC A particle that can move along the x -axis is part of a system with potential energy
U(x)= A/x2 − B/x where A and B are positive constants.
a. Where are the particle's equilibrium positions?
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Textbook Question
A particle moving along the y-axis is in a system with potential energy U = 4y^3 J, where y is in m. What is the -component of the force on the particle at y = 0 m, 1 m, and 2 m?
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Textbook Question
FIGURE EX10.24 is the potential-energy diagram for a 500 g particle that is released from rest at A. What are the particle's speeds at B, C, and D?
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Textbook Question
FIGURE EX10.25 is the potential-energy diagram for a 20 g particle that is released from rest at x = 1.0m. (b) What is the particle's maximum speed? At what position does it have this speed?
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Textbook Question
A stretched spring stores 2.0 J of energy. How much energy will be stored if the spring is stretched three times as far?
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