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Basics of Fluid Mechanics, 2014a

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11.5. NORMAL SHOCK 413<br />

or in a dimensionless form<br />

11.5.3 Operating Equations and Analysis<br />

M ∗ 1 M ∗ 2 = c ∗2 (11.102)<br />

In Figure 11.12, the Mach number after the shock, M y , and the ratio <strong>of</strong> the total<br />

pressure, P 0y /P 0x , are plotted as a function <strong>of</strong> the entrance Mach number. The working<br />

equations were presented earlier. Note that the M y has a minimum value which depends<br />

on the specific heat ratio. It can be noticed that the density ratio (velocity ratio) also<br />

has a finite value regardless <strong>of</strong> the upstream Mach number.<br />

The typical situations in which these equations can be used also include the<br />

moving shocks. The equations should be used with the Mach number (upstream or<br />

downstream) for a given pressure ratio or density ratio (velocity ratio). This kind <strong>of</strong><br />

equations requires examining Table (11.3) for k =1.4 or utilizing Potto-GDC for for<br />

value <strong>of</strong> the specific heat ratio. Finding the Mach number for a pressure ratio <strong>of</strong> 8.30879<br />

and k =1.32 and is only a few mouse clicks away from the following table.<br />

To illustrate the use <strong>of</strong> the<br />

above equations, an example is provided.<br />

Example 11.12:<br />

Air flows with a Mach number <strong>of</strong><br />

M x =3, at a pressure <strong>of</strong> 0.5 [bar] and<br />

a temperature <strong>of</strong> 0 ◦ C goes through a<br />

normal shock. Calculate the temperature,<br />

pressure, total pressure, and velocity<br />

downstream <strong>of</strong> the shock. Assume<br />

that k =1.4.<br />

Solution<br />

Analysis:<br />

First, the known information are<br />

M x = 3, P x = 1.5[bar] and T x =<br />

273K. Using these data, the total<br />

120.0<br />

110.0<br />

100.0<br />

90.0<br />

80.0<br />

70.0<br />

60.0<br />

50.0<br />

40.0<br />

30.0<br />

20.0<br />

10.0<br />

Shock Wave relationship<br />

P y<br />

/P y<br />

, ρ y<br />

/ρ x<br />

and T y<br />

/T x<br />

as a function <strong>of</strong> M x<br />

P y<br />

/P x<br />

T y<br />

/T x<br />

ρ y<br />

/ρ x<br />

0.0<br />

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

Fri Jun 18 15:48:25 2004<br />

M x<br />

Fig. -11.13. The ratios <strong>of</strong> the static properties <strong>of</strong><br />

the two sides <strong>of</strong> the shock.<br />

pressure can be obtained (through an isentropic relationship in Table (11.2), i.e., P 0x<br />

is known). Also with the temperature, T x , the velocity can readily be calculated. The<br />

relationship that was calculated will be utilized to obtain the ratios for the downstream<br />

P x<br />

P 0x<br />

<strong>of</strong> the normal shock. =0.0272237 =⇒ P 0x =1.5/0.0272237 = 55.1[bar]<br />

c x = √ kRT x = √ 1.4 × 287 × 273 = 331.2m/sec<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 />

3.0000 0.47519 2.6790 3.8571 10.3333 0.32834

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