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Modern Engineering Thermodynamics

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86 CHAPTER 3: Thermodynamic Properties<br />

3.11 HOW DO YOU DETERMINE THE “THERMODYNAMIC STATE”?<br />

First, remember that you need the values of only two independent intensive thermodynamic properties to fix the<br />

state of a homogeneous material, and the problem statement always provides these values. Usually, you are<br />

given the values of pressure, temperature, or specific volume in the problem statement. Sometimes specific internal<br />

energy or specific enthalpy also is one of the values given.<br />

Second, choose one of the two given values and look up the corresponding saturation values (f and g) ofthe<br />

other given property from the saturation tables in Thermodynamic Tables to accompany <strong>Modern</strong> <strong>Engineering</strong> <strong>Thermodynamics</strong>,<br />

Tables C.1 and C.2, for your material and compare them with the given value. You can then determine<br />

the state of your material by following the rules in Table 3.9.<br />

For example, if you are given water at a pressure of 1.0 MPa and a temperature of 200.°C, then you could<br />

choose p given = 1.0 MPa and look up T sat at that value of p given . From Table C.1 at p given = 1.0 MPa, you find that<br />

T sat =179.9°C. Since your value of T given =200.°C > T sat =179.9°C, the water must be in a superheated vapor<br />

state. Similarly, if you choose T given = 200.°C instead of p given , then you would look up p sat at that value of T given .<br />

From Table C.1 at T given = 200.°C, you find that p sat = 1.554 MPa. Since your value of p given =1.0 MPa < p sat =<br />

1.554 MPa, you again conclude that the water must be in a superheated vapor state.<br />

While it is true that any pair of independent properties fix the state of a simple substance subjected to only one<br />

work mode, you must be able to deduce the system’s thermodynamic state (compressed liquid, saturated liquid<br />

or vapor, liquid-vapor mixture, or superheated vapor) from the data given in a problem statement to know in<br />

which table to find the other properties required in the analysis. It is important to remember that thermodynamic<br />

states are unique and a given pair of independent properties fix the state at only one point in the tables. It is therefore<br />

essential to understand how to determine which table to use in the solution of a thermodynamics problem.<br />

In Example 3.9, we introduce notation of the form v(X°F, Y psia), which represents the value of the specific<br />

volume evaluated at X°F and Y psia. For example, v(100.°F, 50. psia) means the value of the specific volume at<br />

100.°F and 50. psia. This is a convenient way of recording the pair of independent intensive properties used to<br />

determine the value of v. The same notation is used with the intensive properties u and h.<br />

Table 3.9 How to Find the Thermodynamic “State”<br />

Then You Have a<br />

Properties Given in the<br />

Problem Statement<br />

Choose<br />

Look Up in<br />

Appropriate Table<br />

Compressed<br />

Liquid If<br />

Mixture of Liquid<br />

and Vapor If<br />

Superheated<br />

Vapor If<br />

p given , T given p given T sat at p given T given < T sat T given = T sat T given > T sat<br />

p given , T given T given p sat at T given p given > p sat p given = p sat p given < p sat<br />

p given , υ given<br />

p given<br />

υ f and υ g<br />

υ given < υ f<br />

υ f < υ given < υ g<br />

υ given > υ g<br />

p given , u given<br />

p given<br />

u f and u g<br />

u given < u f<br />

u f < u given < u g<br />

u given > u g<br />

p given , h given<br />

p given<br />

h f and h g<br />

h given < h f<br />

h f < h given < h g<br />

h given > h g<br />

T given , υ given<br />

T given<br />

υ f and υ g<br />

υ given < υ f<br />

υ f < υ given < υ g<br />

υ given > υ g<br />

T given , u given<br />

T given<br />

u f and u g<br />

u given < u f<br />

u f < u given < u g<br />

u given > u g<br />

T given , h given<br />

T given<br />

h f and h g<br />

h given < h f<br />

h f < h given < h g<br />

h given > h g<br />

EXAMPLE 3.9<br />

Find the specific volume and specific enthalpy of Refrigerant-134a at 100.°F<br />

and 95.0 psia (Figure 3.25).<br />

Solution<br />

AcheckofTableC.7aofThermodynamic Tables to accompany <strong>Modern</strong> <strong>Engineering</strong><br />

<strong>Thermodynamics</strong> reveals that the saturation pressure of Refrigerant-134a at<br />

100.°F is 138.83 psia. Since our actual pressure is less than the saturation pressure,<br />

we must have superheated vapor. A check of Table C.8a reveals that<br />

100.°F and 95.0 psia is indeed in the superheated region. However, 95.0 psia<br />

is not a direct entry into this table, so we must use linear interpolation to find<br />

the needed values. This is how a linear interpolation for v is carried out:<br />

FIGURE 3.25<br />

Example 3.9.<br />

R-134a<br />

T = 100.°F<br />

p = 95.0 psia<br />

v = ?<br />

h = ?

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