Chapter 20: Problem 22
Explain how it is possible for a heat pump like that in Example 20.2 to operate with a power of only \(6.28 \mathrm{~kW}\) and heat a house that is losing thermal energy at a rate of \(21.98 \mathrm{~kW}\).
Chapter 20: Problem 22
Explain how it is possible for a heat pump like that in Example 20.2 to operate with a power of only \(6.28 \mathrm{~kW}\) and heat a house that is losing thermal energy at a rate of \(21.98 \mathrm{~kW}\).
All the tools & learning materials you need for study success - in one app.
Get started for freeA Carnot engine takes an amount of heat \(Q_{H}=100 .\) J from a high- temperature reservoir at temperature \(T_{H}=1000 .{ }^{\circ} \mathrm{C},\) and exhausts the remaining heat into a low-temperature reservoir at \(T_{\mathrm{L}}=10.0^{\circ} \mathrm{C}\). Find the amount of work that is obtained from this process.
A proposal is submitted for a novel engine that will operate between \(400 .\mathrm{K}\) and \(300 . \mathrm{K}\). a) What is the theoretical maximum efficiency of the engine? b) What is the total entropy change per cycle if the engine operates at maximum efficiency?
A refrigerator has a coefficient of performance of \(5.00 .\) If the refrigerator absorbs 40.0 cal of heat from the low-temperature reservoir in each cycle, what is the amount of heat expelled into the high-temperature reservoir?
Why might a heat pump have an advantage over a space heater that converts electrical energy directly into thermal energy?
The entropy of a macroscopic state is given by \(S=k_{B} \ln w,\) where \(k_{B}\) is the Boltzmann constant and \(w\) is the number of possible microscopic states. Calculate the change in entropy when \(n\) moles of an ideal gas undergo free expansion to fill the entire volume of a box after a barrier between the two halves of the box is removed.
What do you think about this solution?
We value your feedback to improve our textbook solutions.