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Modern Engineering Thermodynamics

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320 CHAPTER 10: Availability Analysis<br />

CRITICAL THINKING<br />

Is some of the energy with a system “unavailable”? Does the magnitude of the available energy within a system depend on<br />

the accessible technology? What about nuclear energy, is it “available” to do useful work? If not, could future technologies<br />

make it available?<br />

Ground<br />

A<br />

B<br />

C<br />

−h C<br />

More available<br />

energy than B<br />

h A<br />

Less available<br />

h B<br />

energy than A<br />

Unavailable energy<br />

FIGURE 10.1<br />

A system’s available and unavailable energy. The<br />

potential energy of weight A has more “available”<br />

potential energy to do useful work relative to the<br />

ground than does weight B. However, the potential<br />

energy of weight C is negative relative to the<br />

ground and therefore is “unavailable” to do useful<br />

work relative to the ground.<br />

combustion engine can convert only about 20–30% of the chemical energy in its<br />

fuel into useful output work. Therefore, electrical energy is more valuable to our<br />

society than chemical fuel (notice that we have not taken into account how the<br />

electrical energy is generated). Being more valuable, it costs more because it has a<br />

higher “quality” of work “availability.”<br />

Much of the world around us today is driven by various energy conversion technologies.<br />

Automobiles, power plants, manufacturing facilities, and computers are<br />

all important elements in our society today. Since we know that energy is conserved<br />

in all processes, energy would seem to be an inexhaustible resource to be<br />

used over and over again, powering our technological needs. However, though<br />

energy is conserved, it is degraded through use to a form that is not useful in technological<br />

systems. For example, the kinetic energy of a bouncing rubber ball is<br />

continuously degraded by internal friction produced by the deformation of the<br />

ball during impact. This causes the height to which the ball rebounds after each<br />

impact to progressively decrease. Using the second law of thermodynamics, we<br />

can pinpoint where energy degradation occurs within an engineering system; and<br />

by redesigning the system to minimize the energy degradation, we can improve<br />

the overall energy conversion performance of the system.<br />

With increasing material costs and decreasing resources, it is apparent that the<br />

efficient use of energy resources will be of primary importance to engineers in the<br />

future. In engineering design, the concept of pure energy in somewhat misleading.<br />

What a designer needs to know is how much of the energy present in a given system can<br />

be used for a particular process. That is, of the total energy contained within a system, how much is available to do<br />

useful work? Therefore, it is important for engineers to understand how to determine the consequence (i.e., the<br />

amount of useful energy available) of the energy within a given system. The manipulation of the amount of energy<br />

present is the subject of the first law of thermodynamics. The second law of thermodynamics tells us where the<br />

irreversibilities within the system are located (through the entropy production term). If we combine these two<br />

laws and define a new thermodynamic property (called availability) that is a measure of the useful energy, we can<br />

then identify where energy is being degraded or lost within a system and decide how to modify the system to<br />

reduce these losses.<br />

This chapter provides a basic introduction to the availability property and the availability balance. Open and<br />

closed system availability balances are developed, and a new system efficiency based on the second law of thermodynamics<br />

is developed. Examples are presented illustrating the use of this material for power plants, refrigeration<br />

systems, heat pumps, internal combustion engines, and heat exchangers. A summary at the end of the<br />

chapter reiterates the main concepts and equations developed in the chapter.<br />

Useful work is associated with a quantity called the potential of a conservative force. The following section on fields<br />

and forces provides a background on the mathematical nature of fields, potentials, and conservative forces.<br />

10.2 FUN WITH SCALAR, VECTOR, AND CONSERVATIVE FIELDS<br />

10.2.1 Scalar and Vector Fields<br />

A scalar (or vector) function is a mathematical expression defined at each point in a region of space whose resultant<br />

value is a scalar (or vector) quantity that depends only on the point where the expression was evaluated and<br />

not on the coordinate system used. The region of space over which a scalar function is defined is called the scalar<br />

field of the scalar function, and the region of space over which a vector function is defined is called the vector<br />

field of the vector function. For example, the scalar pressure, temperature, and density functions at each point<br />

within an object define the pressure, temperature, and density scalar fields of the object. Similarly, the velocity<br />

vector at each point within a flowing fluid defines the velocity vector field of the fluid.

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