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Basics of Fluid Mechanics, 2014a

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11.7. FANNO FLOW 445<br />

10 2 0 1 2 3 4 5 6 7 8 9 10<br />

10<br />

10 -1 1<br />

4 fL<br />

D<br />

P/P ∗<br />

P 0 /P 0<br />

∗<br />

ρ/ρ ∗<br />

U/U ∗<br />

T/T ∗<br />

10 -2<br />

M<br />

Fig. -11.20. Various parameters in Fanno flow shown as a function <strong>of</strong> Mach number.<br />

11.7.5 Examples <strong>of</strong> Fanno Flow<br />

Example 11.18:<br />

Air flows from a reservoir and enters a uniform pipe with a diameter <strong>of</strong> 0.05 [m] and length <strong>of</strong> 10 [m].<br />

P 0 =?<br />

T 0 =? ◦ C<br />

M 2 =0.9<br />

D=0.05[m]<br />

L=10[m]<br />

T 2 =27 ◦ C<br />

P 2 =1[Bar]<br />

Fig. -11.21. Schematic <strong>of</strong> Example 11.18.<br />

The air exits to the atmosphere.<br />

The following conditions prevail at<br />

the exit: P 2 =1[bar] temperature<br />

T 2 =27 ◦ CM 2 =0.9 23 . Assume<br />

that the average friction factor to<br />

be f =0.004 and that the flow<br />

from the reservoir up to the pipe<br />

inlet is essentially isentropic. Estimate<br />

the total temperature and total pressure in the reservoir under the Fanno flow<br />

model.<br />

Solution<br />

For isentropic, the flow to the pipe inlet, the temperature and the total pressure at the<br />

pipe inlet are the same as those in the reservoir. Thus, finding the star pressure and<br />

temperature at the pipe inlet is the solution. With the Mach number and temperature<br />

known at the exit, the total temperature at the entrance can be obtained by knowing<br />

the 4fL<br />

D<br />

. For given Mach number (M =0.9) the following is obtained.<br />

23 This property is given only for academic purposes. There is no Mach meter.

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