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Basics of Fluid Mechanics, 2014a

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11.10. INTRODUCTION 479<br />

Example 11.23:<br />

Air enters a pipe with pressure <strong>of</strong> 3[bar] and temperature <strong>of</strong> 27 ◦ C at Mach number <strong>of</strong><br />

M =0.25. Due to internal combustion heat was released and the exit temperature was<br />

found to be 127 ◦ C. Calculate the exit Mach number, the exit pressure, the total exit<br />

pressure, and heat released and transferred to the air. At what amount <strong>of</strong> energy the<br />

[<br />

exit temperature will start to decrease? Assume C P =1.004<br />

Solution<br />

kJ<br />

kg ◦ C<br />

The entrance Mach number and the exit temperature are given and from Table (11.7)<br />

or from Potto–GDC the initial ratio can be calculated. From the initial values the ratio<br />

at the exit can be computed as the following.<br />

]<br />

M<br />

T<br />

T ∗ T 0<br />

T 0<br />

∗<br />

P<br />

P ∗ P 0<br />

P 0<br />

∗<br />

ρ ∗ ρ<br />

0.25000 0.30440 0.25684 2.2069 1.2177 0.13793<br />

and<br />

T 2<br />

T ∗ = T 1<br />

T ∗ T 2<br />

T 1<br />

=0.304 × 400<br />

300 =0.4053<br />

M<br />

T<br />

T ∗ T 0<br />

T 0<br />

∗<br />

P<br />

P ∗ P 0<br />

P 0<br />

∗<br />

ρ ∗ ρ<br />

0.29831 0.40530 0.34376 2.1341 1.1992 0.18991<br />

The exit Mach number is known, the exit pressure can be calculated as<br />

P ∗ P 2<br />

P 2 = P 1<br />

P 1 P ∗ =3× 1 × 2.1341 = 2.901[Bar]<br />

2.2069<br />

For the entrance, the stagnation values are<br />

M<br />

T<br />

T 0<br />

ρ<br />

ρ 0<br />

A<br />

A ⋆<br />

P<br />

P 0<br />

A×P<br />

A ∗ ×P 0<br />

F<br />

F ∗<br />

P 02<br />

0.25000 0.98765 0.96942 2.4027 0.95745 2.3005 1.0424<br />

The total exit pressure, P 02 can be calculated as the following:<br />

isentropic<br />

{}}{<br />

P 01<br />

= P 1<br />

P 1<br />

∗<br />

P 0 P 02<br />

∗<br />

P 01 P =3× 1<br />

0 0.95745 × 1 × 1.1992 = 3.08572[Bar]<br />

1.2177<br />

The heat released (heat transferred) can be calculated from obtaining the stagnation<br />

temperature from both sides. The stagnation temperature at the entrance, T 01<br />

T 01<br />

isentropic<br />

{}}{<br />

T 01<br />

= T 1<br />

T 1<br />

= 300/0.98765 = 303.75[K]

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