Chapter 19: Problem 9
Why do refrigerators and heat pumps have different definitions of COP?
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Chapter 19: Problem 9
Why do refrigerators and heat pumps have different definitions of COP?
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A cosmic heat engine might operate between the Sun's \(5800 \mathrm{K}\) surface and the \(2.7 \mathrm{K}\) temperature of intergalactic space. What would be its maximum efficiency?
Find an expression for the entropy gain when hot and cold water are irreversibly mixed. A corresponding reversible process you can use to calculate this change is to bring each water sample slowly to their common final temperature \(T_{\mathrm{f}}\) and then mix them. Express your answer in terms of the initial temperatures \(T_{\mathrm{h}}\) and \(T_{\mathrm{c}} .\) Assume equal masses of hot and cold water, with constant specific heat \(c .\) What's the sign of your answer?
Use appropriate energy-flow diagrams to analyze the situation in GOT IT? \(19.3 ;\) that is, show that using a refrigerator to cool the low-temperature reservoir can't increase the overall efficiency of a Carnot engine when the work input to the refrigerator is included.
A Carnot engine absorbs \(900 \mathrm{J}\) of heat each cycle and provides \(350 \mathrm{J}\) of work. (a) What's its efficiency? (b) How much heat is rejected each cycle? (c) If the engine rejects heat at \(10^{\circ} \mathrm{C}\), what's its maximum temperature?
A shallow pond contains 94 Mg of water. In winter, it's entirely frozen. By how much does the entropy of the pond increase when the ice, already at \(0^{\circ} \mathrm{C}\), melts and then heats to its summer temperature of \(15^{\circ} \mathrm{C} ?\)
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