FUND OF ENG THERMODYN(LLF)+WILEYPLUS
9th Edition
ISBN: 9781119391777
Author: MORAN
Publisher: WILEY
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Figure shows a simple vapor power plant operating at steady state with water as the working fluid. Data at key locations are given on the figure. The mass flow rate of the water circulating through the components is 109 kg/s. Stray heat transfer and kinetic and potential energy effects can be ignored. Determine:
(a) the mass flow rate of the cooling water, in kg/s.
(b) the thermal efficiency.
(c) the rates of entropy production, each in kW/K, for the turbine, condenser, and pump.
(d) Using the results of part (c), place the components in rank order, beginning with the component contributing most to inefficient operation of the overall system. verl
The cycle involved in the operation of an internal combustion engine is called the Otto cycle.
Air can be considered to be the working substance and can be assumed to be a perfect gas. The cycle consists of the following steps:
I) Reversible adiabatic compression from A to B.
2) Reversible constant-volume pressure increase from B to C due to the combustion of a small amount of fuel.
3) Reversible adiabatic expansion from C to D.
4) Reversible and constant-volume pressure decrease back to state A.
Determine the change in entropy (of the system and of the surroundings) for each step of the cycle and determine an expression for the efficiency of the cycle, assuming that the heat is supplied in Step 2. Evaluate the efficiency for a compression ratio 10:1. Assume that in state A, V=4.00 dm', p= 1.00 atm, T= 300 K, that VA = 10 Vb, pc/pb = 5, and that Cp.m = (7/2)R
Note that R = 8.314 J K-1 mol-1 and dm = 10-1 m.
Steam enters the turbine of a power plant operating on the Rankine cycle (Fig. 2) at 873.15 Kand exhausts at 30 kPa. To show the effect of boiler pressure on the performance of the cycle,calculate the thermal efficiency of the cycle and the quality of the exhaust steam from theturbine for boiler pressures of 5000,7500, and 10 000 kPa.
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