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612 Chapter 11 ■ Compressible Flow<br />

maximum entropy difference occurs at a pressure of 2.62 psia and<br />

a temperature of 432.1 °R. p T s s 1<br />

(psia) ( R) [( ft lb) ( lbm R)]<br />

COMMENT Note that for Fanno flow the entropy must increase<br />

in the direction of flow. Hence, this flow can proceed either<br />

from subsonic conditions upstream to a sonic condition 1Ma 12<br />

downstream or from supersonic conditions upstream to a sonic<br />

condition downstream. The arrows in Fig. 11.11 indicate in which<br />

direction a Fanno flow can proceed.<br />

7 502.3 33.6<br />

6 496.8 39.8<br />

5 488.3 46.3<br />

4 474.0 52.6<br />

3 447.7 57.3<br />

2.62 432.1 57.9<br />

2 394.7 55.4<br />

1.8 378.1 53.0<br />

1.5 347.6 47.0<br />

1.4 335.6 44.2<br />

Fanno flow properties<br />

can be obtained<br />

from the second<br />

T ds equation combined<br />

with the continuity<br />

and energy<br />

equations.<br />

We can learn more about Fanno lines by further analyzing the equations that describe the<br />

physics involved. For example, the second T ds equation 1Eq. 11.182 is<br />

For an ideal gas<br />

and<br />

or<br />

T ds dȟ dp<br />

r<br />

dȟ c p dT<br />

r p<br />

RT<br />

dp<br />

p dr r dT<br />

T<br />

Thus, consolidating Eqs. 11.1, 11.7, 11.18, and 11.77 we obtain<br />

T ds c p dT RT a dr r dT T b<br />

Also, from the continuity equation 1Eq. 11.402, we get for Fanno flow rV constant, or<br />

dr<br />

r dV V<br />

(11.18)<br />

(11.7)<br />

(11.1)<br />

(11.77)<br />

(11.78)<br />

(11.79)<br />

Substituting Eq. 11.79 into Eq. 11.78 yields<br />

T ds c p dT RT a dV V dT T b<br />

or<br />

ds<br />

dT c p<br />

T R a1 dV<br />

V dT 1 T b<br />

By differentiating the energy equation 111.742 obtained earlier, we obtain<br />

dV<br />

dT c p<br />

V<br />

(11.80)<br />

(11.81)

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