Chapter 6: Problem 8
How can entropy be transferred into, or out of, a closed system? A control volume?
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Chapter 6: Problem 8
How can entropy be transferred into, or out of, a closed system? A control volume?
These are the key concepts you need to understand to accurately answer the question.
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Get started for freeMethane gas \(\left(\mathrm{CH}_{4}\right)\) enters a compressor at \(298 \mathrm{~K}, 1\) bar and exits at 2 bar and temperature \(T\). Employing the ideal gas model, determine \(T\), in \(\mathrm{K}\), if there is no change in specific entropy from inlet to exit.
An electrically-driven pump operating at steady state draws water from a pond at a pressure of 1 bar and a rate of \(40 \mathrm{~kg} / \mathrm{s}\) and delivers the water at a pressure of 4 bar. There is no significant heat transfer with the surroundings, and changes in kinetic and potential energy can be neglected. The isentropic pump efficiency is \(80 \%\). Evaluating electricity at 8 cents per \(\mathrm{kW} \cdot \mathrm{h}\), estimate the hourly cost of running the pump.
A rigid tank is filled initially with \(5.0 \mathrm{~kg}\) of air at a pressure of \(0.5 \mathrm{MPa}\) and a temperature of \(500 \mathrm{~K}\). The air is allowed to discharge through a turbine into the atmosphere, developing work until the pressure in the tank has fallen to the atmospheric level of \(0.1 \mathrm{MPa}\). Employing the ideal gas model for the air, determine the maximum theoretical amount of work that could be developed, in \(\mathrm{kJ}\). Ignore heat transfer with the atmosphere and changes in kinetic and potential energy.
Complete the following involving reversible and irreversible cycles:
(a) Reversible and irreversible power cycles each discharge energy
\(Q_{\mathrm{C}}\) to a cold reservoir at temperature \(T_{\mathrm{C}}\) and
receive energy \(Q_{\mathrm{H}}\) from hot reservoirs at temperatures
\(T_{\mathrm{H}}\) and \(T_{\mathrm{H}}^{\prime}\), respectively. There are no
other heat transfers. Show that \(T_{\mathrm{H}}^{\prime}>T_{\mathrm{H}}\).
(b) Reversible and irreversible refrigeration cycles each discharge energy
\(Q_{\mathrm{H}}\) to a hot reservoir at temperature \(T_{\mathrm{H}}\) and
receive energy \(Q_{C}\) from cold reservoirs at temperatures \(T_{C}\). and
\(T_{C}^{\prime}\), respectively. There are no other heat transfers. Show that
\(T_{\mathrm{C}}^{\prime}>T_{\mathrm{C}}\).
(c) Reversible and irreversible heat pump cycles each receive energy
\(Q_{\mathrm{C}}\) from a cold reservoir at temperature \(T_{\mathrm{C}}\) and
discharge energy \(Q_{\mathrm{H}}\) to hot reservoirs at temperatures
\(T_{\mathrm{H}}\) and \(T_{\mathrm{H}}^{\prime}\), respectively. There are no
other heat transfers. Show that \(T_{\mathrm{H}}^{\prime}
Air enters an insulated compressor operating at steady state at 1 bar, \(350 \mathrm{~K}\) with a mass flow rate of \(1 \mathrm{~kg} / \mathrm{s}\) and exits at 4 bar. The isentropic compressor efficiency is \(82 \%\). Determine the power input, in \(\mathrm{kW}\), and the rate of entropy production, in \(\mathrm{kW} / \mathrm{K}\), using the ideal gas model with (a) data from Table A-22. (b) \(I T\). (c) a constant specific heat ratio, \(k=1.39\).
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