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Modern Engineering Thermodynamics

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74 CHAPTER 3: Thermodynamic Properties<br />

Pressure, p<br />

x = 0<br />

v g − v f<br />

Critical point<br />

Actual<br />

state<br />

x = 1<br />

Equation (3.21) is just a simple mass-based lever rule equation<br />

relating a mixture thermodynamic property (v) tothethermodynamic<br />

properties of the components of the mixture (v f and<br />

v g ). We now define the quality x of a liquid plus vapor mixture<br />

as the relative amount of vapor present, or<br />

Quality = x =<br />

Mass of vapor<br />

Mass of vapor<br />

=<br />

Mass of vapor + Mass of liquid Total mass<br />

v − v f<br />

or<br />

v f<br />

v v g<br />

Specific volume, v<br />

FIGURE 3.16<br />

The lever rule for calculating quality.<br />

m g<br />

x =<br />

m f + m g<br />

Therefore, Eq. (3.21) can be written as<br />

which can be rearranged as<br />

where we define the magnitude of the liquid to vapor property change as<br />

From Figure 3.16, we see that another definition of quality is<br />

= m g<br />

m<br />

(3.22)<br />

v = ð1 − xÞv f + xv g (3.23)<br />

v = v f + xðv g − v f Þ = v f + xv fg (3.24)<br />

v fg = v g − v f (3.25)<br />

x = v − v f<br />

v fg<br />

(3.26)<br />

It should be clear from the definition of quality that its value has the following bounds<br />

Saturated liquid : x = 0<br />

Saturated vapor : x = 1<br />

Wet ðliquid plus vaporÞ region : 0 < x < 1<br />

WHY DO THEY CALL IT QUALITY?<br />

In the 19th century, there were a lot of steam engines.<br />

Railroads, factories, ships, and so on all used steam engines<br />

as their source of power. The people responsible for keeping<br />

these engines running noticed that they worked better if the<br />

steam contained more vapor than liquid. So, a mixture that<br />

contained a lot of vapor and little liquid was said to be of<br />

high quality. Theydefinedthisquality to be the ratio of the<br />

mass of vapor to total mass of liquid plus vapor (Figure<br />

3.17), or quality = x = m g /(m f + m g )=m g /m. Ontheother<br />

hand, the amount of liquid present in a mixture is called<br />

the moisture of the mixture, defined as moisture = m f /m =<br />

1 − x. Since these definitions apply only to mixtures of<br />

liquid plus vapor, they do not extend outside of the vapor<br />

dome. The condition where the quality x =1.0isreserved<br />

for saturated vapor and does not apply to superheated<br />

vapor. Similarly, the condition where quality x =0 is<br />

reserved for saturated liquid and does not apply to compressed<br />

liquid. Note that the quality x of a liquid-vapor mixture<br />

can never be less than 0 or greater than 1.0. That is, x<br />

always falls in the range 0 < x < 1.0.<br />

Vapor<br />

Liquid<br />

High quality,<br />

low moisture<br />

Vapor<br />

Liquid<br />

Low quality,<br />

high moisture<br />

FIGURE 3.17<br />

Why do they call it quality? In all other single-phase regions<br />

(compressed liquid, superheated vapor, gaseous), x is not defined,<br />

because these are single-phase homogeneous regions. Note that,<br />

since the numerical value of quality is restricted to lie in the range<br />

from 0 to 1, no correct calculation can ever give a value of x less<br />

than 0 or greater than 1.0.

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