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Modern Engineering Thermodynamics

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198 CHAPTER 6: First Law Open System Applications<br />

2. The general open system energy rate balance (ERB) equation:<br />

_Q − _W +∑ _m h+ V 2 <br />

/2g c + gZ/g c − ∑ _m h+ V 2 <br />

/2g c + gZ/g c<br />

inlet<br />

outlet<br />

(6.4)<br />

= d dt<br />

U + mV 2 /2g c + mgZ/g c<br />

system<br />

3. The modified open system energy rate balance equation:<br />

_Q − _W + _m½h in − h out + ðV 2 in − V2 out Þ/ð2g cÞ + ðZ in − Z out Þðg/g c ÞŠ = 0 (6.12)<br />

Other equations are developed in this chapter that apply to specific geometries and boundary conditions. These<br />

equations are best studied in the context of the specific examples in which they were developed. The secret to<br />

mastering this material is to become competent at developing the equations that fit your specific problem by<br />

starting from the basic energy and auxiliary equations and applying the relevant boundary conditions (adiabatic,<br />

negligible kinetic or potential energies, and so forth). Consequently, not all the equations developed in this<br />

chapter are listed here so that you are encouraged to learn how to use the basic equations by studying the example<br />

problems and solutions presented.<br />

The example problems discussed in this chapter are not meant to cover all the possible aspects of open<br />

system energy analysis. They were chosen to illustrate the problem solving technique, thermodynamic<br />

table usage, and how to make basic assumptions about process variables. You must learn how to successfully<br />

apply a generalized problem solution technique, such as the one used in this chapter and illustrated in<br />

the flowchart of Figure 4.21. More problem solving skills are gained by doing the problems at the end of<br />

this chapter.<br />

Table 6.5 lists some of the new technical thermodynamic terms introduced in this chapter and earlier chapters.<br />

These terms are used without further explanation in the chapters that follow. It is recommended that the student<br />

learn their definitions before proceeding to the next chapter.<br />

Table 6.5 Glossary of Technical Terms Introduced in Chapter 6 and Earlier Chapters<br />

EB<br />

The energy balance<br />

ERB<br />

The energy rate balance<br />

1Q 2 and Q _ Heat transfer and heat transfer rate<br />

1W 2 and W _ Work and work rate (power)<br />

Aergonic<br />

No work<br />

Reversible work<br />

No losses (i.e., no friction, heat transfer, etc.)<br />

Work efficiency<br />

A measure of the losses within a machine<br />

Coefficient of performance (COP) The name we give energy conversion efficiency when it is more than 100%<br />

Conduction heat transfer<br />

The heat transport of energy that obeys Fourier’s law<br />

Convection heat transfer<br />

The heat transport of energy that obeys Newton’s law of cooling<br />

Radiation heat transfer<br />

The heat transport of energy that obeys the Stefan-Boltzmann law<br />

Adiabatic<br />

No heat transfer<br />

Steady state<br />

A thermodynamic state that is constant in time<br />

Steady flow<br />

A state wherein the mass of an open system is constant in time<br />

Flow stream<br />

Where mass crosses a system boundary<br />

Station<br />

A data monitoring point on a flow stream<br />

MEB<br />

The modified energy balance<br />

MERB<br />

The modified energy rate balance<br />

Pressure energy<br />

Sometimes called the pressure head, _mpv<br />

Nozzle<br />

A device for converting pressure energy into kinetic energy<br />

Diffuser<br />

A device for converting kinetic energy into pressure energy<br />

Heat exchanger<br />

A device for promoting heat transfer from one fluid to another

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