10.07.2015 Views

Thermodynamics

Thermodynamics

Thermodynamics

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

Chapter 8 | 427installed power), the highest efficiency of a wind turbine is about 59 percent.In practice, the actual efficiency ranges between 20 and 40 percent and isabout 35 percent for many wind turbines.Wind power is suitable for harvesting when there are steady winds with anaverage velocity of at least 6 m/s (or 13 mph). Recent improvements inwind turbine design have brought the cost of generating wind power toabout 5 cents per kWh, which is competitive with electricity generated fromother resources.EXAMPLE 8–2Exergy Transfer from a FurnaceConsider a large furnace that can transfer heat at a temperature of 2000 Rat a steady rate of 3000 Btu/s. Determine the rate of exergy flow associatedwith this heat transfer. Assume an environment temperature of 77°F.Solution Heat is being supplied by a large furnace at a specified temperature.The rate of exergy flow is to be determined.Analysis The furnace in this example can be modeled as a heat reservoirthat supplies heat indefinitely at a constant temperature. The exergy of thisheat energy is its useful work potential, that is, the maximum possibleamount of work that can be extracted from it. This corresponds to theamount of work that a reversible heat engine operating between the furnaceand the environment can produce.The thermal efficiency of this reversible heat engine ish th,max h th,rev 1 T L 1 T 0 1 537 RT H T H 2000 R 0.732 1or 73.2% 2That is, a heat engine can convert, at best, 73.2 percent of the heat receivedfrom this furnace to work. Thus, the exergy of this furnace is equivalent tothe power produced by the reversible heat engine:W # max W # rev h th,rev Q # Totalenergyin 10.732213000 Btu>s2 2196 Btu/sDiscussion Notice that 26.8 percent of the heat transferred from the furnaceis not available for doing work. The portion of energy that cannot beconverted to work is called unavailable energy (Fig. 8–7). Unavailable energyis simply the difference between the total energy of a system at a specifiedstate and the exergy of that energy.UnavailableenergyExergyFIGURE 8–7Unavailable energy is the portion ofenergy that cannot be converted towork by even a reversible heat engine.8–2 ■ REVERSIBLE WORK AND IRREVERSIBILITYThe property exergy serves as a valuable tool in determining the quality ofenergy and comparing the work potentials of different energy sources or systems.The evaluation of exergy alone, however, is not sufficient for studyingengineering devices operating between two fixed states. This is because whenevaluating exergy, the final state is always assumed to be the dead state,which is hardly ever the case for actual engineering systems. The isentropicefficiencies discussed in Chap. 7 are also of limited use because the exit stateINTERACTIVETUTORIALSEE TUTORIAL CH. 8, SEC. 2 ON THE DVD.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!