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Basics of Fluid Mechanics, 2014a

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508 CHAPTER 12. COMPRESSIBLE FLOW 2–DIMENSIONAL<br />

12.2.3 Application <strong>of</strong> Oblique Shock<br />

α 1<br />

α 2<br />

α 3<br />

normal shock<br />

oblique shock<br />

Fig. -12.13.<br />

Two variations <strong>of</strong> inlet suction for supersonic flow.<br />

One <strong>of</strong> the practical applications <strong>of</strong> the oblique shock is the design <strong>of</strong> an inlet<br />

suction for a supersonic flow. It is suggested that a series <strong>of</strong> weak shocks should replace<br />

one normal shock to increase the efficiency (see Figure (12.13)) 17 . Clearly, with a proper<br />

design, the flow can be brought to a subsonic flow just below M =1. In such a case,<br />

there is less entropy production (less pressure loss). To illustrate the design significance<br />

<strong>of</strong> the oblique shock, the following example is provided.<br />

Example 12.5:<br />

The Section described in Figure 12.13 and<br />

12.14 air is flowing into a suction section<br />

at M = 2.0, P = 1.0[bar], and<br />

T =17 ◦ C. Compare the different conditions<br />

in the two different configurations.<br />

Assume that only a weak shock occurs.<br />

α 1<br />

7 ◦<br />

ÓÐÕÙ ×Ó×<br />

1<br />

2 3 4<br />

« ¾ 7 ◦<br />

neglect<br />

the detached<br />

distance<br />

Normal shock<br />

Solution<br />

Fig. -12.14. Schematic for Example (12.5).<br />

The first configuration is <strong>of</strong> a normal shock for which the results 18 are<br />

M x M y<br />

T y<br />

T x<br />

ρ y<br />

ρ x<br />

P y<br />

P x<br />

P 0y<br />

P 0x<br />

2.0000 0.57735 1.6875 2.6667 4.5000 0.72087<br />

17 In fact, there is general pro<strong>of</strong> that regardless to the equation <strong>of</strong> state (any kind <strong>of</strong> gas), the entropy<br />

is to be minimized through a series <strong>of</strong> oblique shocks rather than through a single normal shock. For<br />

details see Henderson and Menik<strong>of</strong>f “Triple Shock Entropy Theorem,” Journal <strong>of</strong> <strong>Fluid</strong> <strong>Mechanics</strong> 366,<br />

(1998) pp. 179–210.<br />

18 The results in this example are obtained using the graphical interface <strong>of</strong> POTTO–GDC thus, no<br />

input explanation is given. In the past the input file was given but the graphical interface it is no longer<br />

needed.

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