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Basics of Fluid Mechanics, 2014a

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12.2. OBLIQUE SHOCK 519<br />

From these tables the pressure ratio at zone 3 and 4 can be calculated<br />

P 3<br />

= P 3 P 2 P 0 P 1<br />

1 1<br />

=1.6247 × 1.9791<br />

P 4 P 2 P 0 P 1 P 4 1.6963 1.6038 ∼ 1.18192<br />

To reduce the pressure ratio the deflection angle has to be reduced (remember that at<br />

weak weak shock almost no pressure change). Thus, the pressure at zone 3 has to be<br />

reduced. To reduce the pressure the angle <strong>of</strong> slip plane has to increase from 1.5◦ to a<br />

larger number.<br />

End Solution<br />

Example 12.15:<br />

The previous example gave rise to another question on the order <strong>of</strong> the deflection angles.<br />

Consider the same values as previous analysis, will the oblique shock with first angle <strong>of</strong><br />

15 ◦ and then 12 ◦ or opposite order make a difference (M =5)? If not what order will<br />

make a bigger entropy production or pressure loss? (No general pro<strong>of</strong> is needed).<br />

Solution<br />

Waiting for the solution<br />

End Solution<br />

12.2.3.1 Retouch <strong>of</strong> Shock Drag or Wave Drag<br />

Since it was established that the common<br />

explanation is erroneous and the steam<br />

lines are bending/changing direction when<br />

they touching the oblique shock (compare<br />

with figure (11.15)). The correct explanation<br />

is that increase <strong>of</strong> the momentum into<br />

control volume is either requires increase<br />

<strong>of</strong> the force and/or results in acceleration<br />

<strong>of</strong> gas. So, what is the effects <strong>of</strong> the<br />

oblique shock on the Shock Drag? Figure<br />

(12.19) exhibits schematic <strong>of</strong> the oblique<br />

shock which show clearly that stream lines<br />

are bended. There two main points that<br />

should be discussed in this context are the<br />

stationary control<br />

volume<br />

U 1 = 0 U 1 ≠ 0<br />

ρ ρ 1 2<br />

A 1 A 2<br />

P 1<br />

P 2<br />

stream lines<br />

moving<br />

object<br />

Fig. -12.19. The diagram that explains the<br />

shock drag effects <strong>of</strong> a moving shock considering<br />

the oblique shock effects.<br />

additional effects and infinite/final structure. The additional effects are the mass start<br />

to have a vertical component. The vertical component one hand increase the energy<br />

needed and thus increase need to move the body (larger shock drag) (note the there<br />

is a zero momentum net change for symmetrical bodies.). However, the oblique shock<br />

reduces the normal component that undergoes the shock and hence the total shock<br />

drag is reduced. The oblique shock creates a finite amount <strong>of</strong> drag (momentum and<br />

energy lost) while a normal shock as indirectly implied in the common explanation creates<br />

de facto situation where the shock grows to be infinite which <strong>of</strong> course impossible.

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