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Basics of Fluid Mechanics, 2014a

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6.1. MOMENTUM GOVERNING EQUATION 177<br />

The velocity pr<strong>of</strong>ile is<br />

U<br />

( r<br />

) [ ( r<br />

) ] 2<br />

= U max 1 −<br />

R R<br />

(6.I.a)<br />

Substituting equation (6.I.a) into equation (6.18)<br />

results in<br />

Thus,<br />

U 2 = 1 ∫ R<br />

2 πR 2 [U(r)] 2 2 πrdr<br />

U 2 =(U max ) 2 ∫ 1<br />

0<br />

0<br />

(6.I.b)<br />

(<br />

1 − ¯r<br />

2 ) 2<br />

¯rd¯r =<br />

1<br />

6 (U max) 2 (6.I.c)<br />

U = U max<br />

√<br />

6<br />

End Solution<br />

U i<br />

y<br />

x<br />

U o<br />

θ<br />

U o<br />

F<br />

U i<br />

F<br />

Fig a. Schematics <strong>of</strong> area impinged by a jet<br />

for example 6.2.<br />

Fig b. Schematics <strong>of</strong> maximum angle for<br />

impinged by a jet.<br />

Fig. -6.2. Schematics <strong>of</strong> area impinged by a jet and angle effects.<br />

Example 6.2:<br />

A jet is impinging on a stationary surface by changing only the jet direction (see Figure<br />

6.2). Neglect the friction, calculate the force and the angle which the support has to<br />

apply to keep the system in equilibrium. What is the angle for which maximum force<br />

will be created?<br />

Solution<br />

Equation (6.11) can be reduced, because it is a steady state, to<br />

∫<br />

F =<br />

out<br />

ρU<br />

U { }}<br />

rn<br />

{ ∫ U { }}<br />

rn<br />

{<br />

(U · ˆn) dA − ρU (U · ˆn) dA = ṁU U o − ṁU U i<br />

in<br />

(6.II.a)

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