1. Steve, with mass m, is ready to squat jump Kale’s insecurities—represented by n moles of a solid with total mass M—out of Earth’s atmosphere. He decides to model his squat as a spring with constant k compressing vertically down a distance d from equilibrium, and the jump as releasing that spring, launching himself and Kale’s insecurities to a maximum height h above equilibrium. He does everything perfectly.
a) When he gets to that maximum height, he finds that Kale’s insecurities have heated by ∆T. How much energy went into heating them ?.
b) Assuming Steve’s temperature did not change and no other interactions were present, how far did Steve compress his model spring?
Atoms in solids have 3 degrees of freedom
Internal energy of solids Ein = 3nRT
when the temperature of Kale's has raised by T
change in internal energy = 3nR T - energy taken to heat Kale's
R = 8.31 J/mole/K - gas const.
b) Steve and Kale have gone to a height h
change in PE = (m+M)gh
if the spring is compressed by d , PE stored in the spring = kd2/2
Total spring energy is used to raise them by a height h and heating up Kale's, there are no other interactions. Conserving the total energy
kd2 = (m+M)gh + 3nR T
compression of spring
d = { ( (m+M)gh + 3nR T )/k }1/2
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