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Show that the thermal efficiency of a combined gas-steam power plant \(\eta_{\mathrm{cc}}\) can be expressed as $$\eta_{\mathrm{cc}}=\eta_{g}+\eta_{s}-\eta_{g} \eta_{s}$$ where \(\eta_{g}=W_{g} / Q_{\text {in }}\) and \(\eta_{s}=W_{s} / Q_{g, \text { out }}\) are the thermal efficiencies of the gas and steam cycles, respectively. Using this relation, determine the thermal efficiency of a combined power cycle that consists of a topping gas-turbine cycle with an efficiency of 40 percent and a bottoming steam-turbine cycle with an efficiency of 30 percent.

Short Answer

Expert verified
To summarize, we derived the formula for the combined cycle's thermal efficiency as: $$\eta_{cc} = \eta_g + \eta_s - \eta_g\eta_s$$ Then, we calculated the thermal efficiency of the given combined power cycle with gas-turbine cycle efficiency of 0.4 and steam-turbine cycle efficiency of 0.3. The combined cycle's thermal efficiency was found to be 58% (0.58).

Step by step solution

01

Deriving the formula for the combined cycle's thermal efficiency

We will use the definitions of thermal efficiency and the energy balance for a combined cycle to derive the given formula. For a combined cycle: $$Q_{in} = Q_{in_g} + Q_{in_s} = Q_{out_g} + Q_{out_s}$$ The thermal efficiencies of the gas-turbine cycle and the steam-turbine cycle are given as: $$\eta_g = \frac{W_g}{Q_{in_g}}$$ $$\eta_s = \frac{W_s}{Q_{out_g}}$$ The efficiency of the combined cycle is: $$\eta_{cc} = \frac{W_{cc}}{Q_{in}}$$ Where \(W_{cc}\) is the total work of the combined cycle. Now let's express the cycle's work in terms of known parameters: $$W_{cc} = W_g + W_s$$ Using first thermal efficiency equation, $$W_g = \eta_g Q_{in_g}$$ Using second thermal efficiency equation, $$W_s = \eta_s Q_{out_g}$$ Substitute these into the combined cycle's work equation: $$W_{cc} = \eta_g Q_{in_g} + \eta_s Q_{out_g}$$ Now, we need to express \(Q_{out_g}\) in terms of \(Q_{in_g}\): $$Q_{out_g} = Q_{in_g} - W_g = Q_{in_g}(1 - \eta_g)$$ Substitute this into \(W_{cc}\): $$W_{cc} = \eta_g Q_{in_g} + \eta_s Q_{in_g}(1 - \eta_g)$$ Now substitute this into the combined cycle's thermal efficiency equation: $$\eta_{cc} = \frac{\eta_g Q_{in_g} + \eta_s Q_{in_g}(1 - \eta_g)}{Q_{in}}$$ Since \(Q_{in} = Q_{in_g}\), $$\eta_{cc} = \eta_g + \eta_s - \eta_g\eta_s$$ Therefore, we have derived the required formula. Now, let's compute the thermal efficiency of the given combined power cycle.
02

Calculating the thermal efficiency of the given combined power cycle

We are given that the gas-turbine cycle efficiency \(\eta_g\) is 40% (0.4) and the steam-turbine cycle efficiency \(\eta_s\) is 30% (0.3). Using the derived formula, we can calculate the combined cycle's thermal efficiency: $$\eta_{cc} = \eta_g + \eta_s - \eta_g\eta_s = 0.4 + 0.3 - (0.4)(0.3)$$ $$\eta_{cc} = 0.4 + 0.3 - 0.12 = 0.58$$ So the thermal efficiency of the combined power cycle is 58% (0.58).

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Most popular questions from this chapter

A large food-processing plant requires \(1.5 \mathrm{lbm} / \mathrm{s}\) of saturated or slightly superheated steam at 140 psia, which is extracted from the turbine of a cogeneration plant. The boiler generates steam at 800 psia and \(1000^{\circ} \mathrm{F}\) at a rate of \(10 \mathrm{lbm} / \mathrm{s}\) and the condenser pressure is 2 psia. Steam leaves the process heater as a saturated liquid. It is then mixed with the feedwater at the same pressure and this mixture is pumped to the boiler pressure. Assuming both the pumps and the turbine have isentropic efficiencies of 86 percent, determine \((a)\) the rate of heat transfer to the boiler and ( \(b\) ) the power output of the cogeneration plant.

Consider an ideal reheat-regenerative Rankine cycle with one open feedwater heater. The boiler pressure is \(10 \mathrm{MPa}\), the condenser pressure is \(15 \mathrm{kPa}\), the reheater pressure is \(1 \mathrm{MPa}\), and the feedwater pressure is \(0.6 \mathrm{MPa}\). Steam enters both the high- and low- pressure turbines at \(500^{\circ} \mathrm{C} .\) Show the cycle on a \(T\) -s diagram with respect to saturation lines, and determine (a) the fraction of steam extracted for regeneration and \((b)\) the thermal efficiency of the cycle.

Steam enters the turbine of a steam power plant that operates on a simple ideal Rankine cycle at a pressure of \(6 \mathrm{MPa},\) and it leaves as a saturated vapor at \(7.5 \mathrm{kPa}\). Heat is transferred to the steam in the boiler at a rate of \(40,000 \mathrm{kJ} / \mathrm{s}\) Steam is cooled in the condenser by the cooling water from a nearby river, which enters the condenser at \(15^{\circ} \mathrm{C}\). Show the cycle on a \(T-s\) diagram with respect to saturation lines, and determine \((a)\) the turbine inlet temperature, \((b)\) the net power output and thermal efficiency, and \((c)\) the minimum mass flow rate of the cooling water required.

Using EES (or other) software, investigate the effect of the boiler pressure on the performance of a simple ideal Rankine cycle. Steam enters the turbine at \(500^{\circ} \mathrm{C}\) and exits at \(10 \mathrm{kPa}\). The boiler pressure is varied from 0.5 to 20 MPa. Determine the thermal efficiency of the cycle and plot it against the boiler pressure, and discuss the results.

Using EES (or other) software, investigate the effect of the condenser pressure on the performance of a simple ideal Rankine cycle. Turbine inlet conditions of steam are maintained constant at \(10 \mathrm{MPa}\) and \(550^{\circ} \mathrm{C}\) while the condenser pressure is varied from 5 to 100 kPa. Determine the thermal efficiency of the cycle and plot it against the condenser pressure, and discuss the results.

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