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Basics of Fluid Mechanics, 2014a

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194 CHAPTER 6. MOMENTUM CONSERVATION<br />

Equation (6.VII.a) can be written as<br />

m l (t) =m l0 −<br />

∫ t<br />

0<br />

U e A e dt<br />

(6.VII.j)<br />

From equation (6.VII.a) it also can be written that<br />

dh l<br />

dt = U e A e<br />

ρ e A<br />

(6.VII.k)<br />

According to the assumption the flow out is linear function <strong>of</strong> the pressure inside thus,<br />

U e = f(P )+gh l rho ⋍ f(P )=ζP<br />

(6.VII.l)<br />

Where ζ here is a constant which the right units.<br />

The liquid momentum balance is<br />

−g (m R + m l ) − a (m R + m l )=<br />

=0<br />

{ }} {<br />

d<br />

dt (m R + m l ) U +bc +(U R + U l ) m l<br />

(6.VII.m)<br />

Where bc is the change <strong>of</strong> the liquid mass due the boundary movement.<br />

End Solution<br />

Example 6.8:<br />

A rocket is filled with only compressed gas. At a specific moment the valve is opened<br />

and the rocket is allowed to fly. What is the minimum pressure which make the rocket<br />

fly. What are the parameters that effect the rocket velocity. Develop an expression for<br />

the rocket velocity.<br />

Example 6.9:<br />

In Example 6.5 it was mentioned that there are only two velocity components. What<br />

was the assumption that the third velocity component was neglected.<br />

6.4.1 Qualitative Questions<br />

Example 6.10:<br />

For each following figures discuss and state force direction and the momentum that act<br />

on the control volume due to .<br />

Example 6.11:

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