Chapter 8: Problem 23
Show that the power produced by a wind turbine is proportional to the cube of the wind velocity and to the square of the blade span diameter.
Chapter 8: Problem 23
Show that the power produced by a wind turbine is proportional to the cube of the wind velocity and to the square of the blade span diameter.
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Get started for freeIn order to cool 1 ton of water at \(20^{\circ} \mathrm{C}\) in an insulated tank, a person pours \(80 \mathrm{kg}\) of ice at \(-5^{\circ} \mathrm{C}\) into the water. Determine ( \(a\) ) the final equilibrium temperature in the \(\operatorname{tank}\) and \((b)\) the exergy destroyed during this process. The melting temperature and the heat of fusion of ice at atmospheric pressure are \(0^{\circ} \mathrm{C}\) and \(333.7 \mathrm{kJ} / \mathrm{kg}\), respectively. Take \(T_{0}=20^{\circ} \mathrm{C}\).
\Air enters a compressor at ambient conditions of 15 psia and \(60^{\circ} \mathrm{F}\) with a low velocity and exits at 150 psia, \(620^{\circ} \mathrm{F},\) and \(350 \mathrm{ft} / \mathrm{s}\). The compressor is cooled by the ambient air at \(60^{\circ} \mathrm{F}\) at a rate of \(1500 \mathrm{Btu} / \mathrm{min} .\) The power input to the compressor is 400 hp. Determine \((a)\) the mass flow rate of air and \((b)\) the portion of the power input that is used just to overcome the irreversibilities.
A \(40-\mathrm{ft}^{3}\) adiabatic container is initially evacuated. The supply line contains air that is maintained at 150 psia and \(90^{\circ} \mathrm{F}\). The valve is opened until the pressure in the container is the same as the pressure in the supply line. Determine the work potential of the air in this container when it is filled. Take \(T_{0}=80^{\circ} \mathrm{F}\).
Steam is throttled from 7 MPa and \(500^{\circ} \mathrm{C}\) to a pressure of 1 MPa. Determine the decrease in exergy of the steam during this process. Assume the surroundings to be at \(25^{\circ} \mathrm{C} .\)
A heat engine receives heat from a source at \(1500 \mathrm{K}\) at a rate of \(600 \mathrm{kJ} / \mathrm{s}\) and rejects the waste heat to a sink at \(300 \mathrm{K} .\) If the power output of the engine is \(400 \mathrm{kW}\), the second-law efficiency of this heat engine is \((a) 42 \%\) (b) \(53 \%\) \((c) 83 \%\) \((d) 67 \%\) \((e) 80 \%\)
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