Chapter 19: Problem 51
The temperature of \(n\) moles of ideal gas is changed from \(T_{1}\) to \(T_{2}\) at constant volume. Show that the corresponding entropy change is \(\Delta S=n C_{V} \ln \left(T_{2} / T_{1}\right)\).
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Chapter 19: Problem 51
The temperature of \(n\) moles of ideal gas is changed from \(T_{1}\) to \(T_{2}\) at constant volume. Show that the corresponding entropy change is \(\Delta S=n C_{V} \ln \left(T_{2} / T_{1}\right)\).
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A Carnot engine absorbs \(950 \mathrm{~J}\) of heat each cycle and provides \(360 \mathrm{~J}\) 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?
In an adiabatic free expansion, \(6.36\) mol of ideal gas at \(305 \mathrm{~K}\) expands 15 -fold in volume. How much energy becomes unavailable to do work?
A box containing 10 coins lying heads up is found to have only 5 coins heads up after shaking. Is there any positive entropy change?
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?
Toyota's Mirai fuel-cell car stores its hydrogen \(\left(\mathrm{H}_{2}\right)\) fuel in tanks that hold \(5.0 \mathrm{~kg}\) of hydrogen at \(70 \mathrm{MPa}\) pressure. During a test one of these tanks leaks its hydrogen into the surrounding test chamber, whose volume is \(955 \mathrm{~m}^{3}\) and which is essentially at vacuum. The hydrogen stays at a constant \(293-\mathrm{K}\) temperature during this process. If the energy that becomes unavailable to do work is \(54.6 \mathrm{MJ}\), what's the fuel tank's volume? Note: The unavailable energy here is not the energy that would have been released on reacting the hydrogen in the vehicle's fuel cell; rather, it's the much lower energy that could have been recovered by using the pressurized gas to turn a turbine.
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