Chapter 8: Problem 3
How does useful work differ from actual work? For what kind of systems are these two identical?
Chapter 8: Problem 3
How does useful work differ from actual work? For what kind of systems are these two identical?
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Get started for freeAn ordinary egg can be approximated as a \(5.5-\mathrm{cm}-\) diameter sphere. The egg is initially at a uniform temperature of \(8^{\circ} \mathrm{C}\) and is dropped into boiling water at \(97^{\circ} \mathrm{C}\). Taking the properties of egg to be \(\rho=1020 \mathrm{kg} / \mathrm{m}^{3}\) and \(c_{p}=3.32 \mathrm{kJ} / \mathrm{kg} \cdot^{\circ} \mathrm{C}\) determine how much heat is transferred to the egg by the time the average temperature of the egg rises to \(70^{\circ} \mathrm{C}\) and the amount of exergy destruction associated with this heat transfer process. Take \(T_{0}=25^{\circ} \mathrm{C}\).
Liquid water enters an adiabatic piping system at \(15^{\circ} \mathrm{C}\) at a rate of \(3 \mathrm{kg} / \mathrm{s}\). It is observed that the water temperature rises by \(0.3^{\circ} \mathrm{C}\) in the pipe due to friction. If the environment temperature is also \(15^{\circ} \mathrm{C}\), the rate of exergy destruction in the pipe is \((a) 3.8 \mathrm{kW}\) (b) \(24 \mathrm{kW}\) \((c) 72 \mathrm{kW}\) \((d) 98 \mathrm{kW}\) \((e) 124 \mathrm{kW}\)
Refrigerant- 134 a is converted from a saturated liquid to a saturated vapor in a closed system using a reversible constant pressure process by transferring heat from a heat reservoir at \(6^{\circ} \mathrm{C}\). From second-law point of view, is it more effective to do this phase change at \(100 \mathrm{kPa}\) or \(180 \mathrm{kPa} ?\) Take \(T_{0}=25^{\circ} \mathrm{C}\) and \(P_{0}=100 \mathrm{kPa}\).
Steamexpands in a turbine steadily at arate of $$18,000 \mathrm{kg} / \mathrm{h}$$ entering at \(7 \mathrm{MPa}\) and \(600^{\circ} \mathrm{C}\) and leaving at \(50 \mathrm{kPa}\) as saturated vapor. Assuming the surroundings to be at \(100 \mathrm{kPa}\) and \(25^{\circ} \mathrm{C},\) determine \((a)\) the power potential of the steam at the inlet conditions and \((b)\) the power output of the turbine if there were no irreversibilities present.
The radiator of a steam heating system has a volume of \(20 \mathrm{L}\) and is filled with superheated water vapor at \(200 \mathrm{kPa}\) and \(200^{\circ} \mathrm{C}\). At this moment both the inlet and the exit valves to the radiator are closed. After a while it is observed that the temperature of the steam drops to \(80^{\circ} \mathrm{C}\) as a result of heat transfer to the room air, which is at \(21^{\circ} \mathrm{C}\). Assuming the surroundings to be at \(0^{\circ} \mathrm{C}\), determine ( \(a\) ) the amount of heat transfer to the room and \((b)\) the maximum amount of heat that can be supplied to the room if this heat from the radiator is supplied to a heat engine that is driving a heat pump. Assume the heat engine operates between the radiator and the surroundings.
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