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Mechanics of Fluids

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The pressure diagrams show that for the next step (B changed<br />

from 0.08 to 0.06) the 13.61 m wave returns and the corresponding<br />

pressure rise at the valve changes sign. The table then<br />

continues:<br />

B (m 1/2 · s −1 ) Head at valve, h (m) u (m · s −1 ) �h (m)<br />

0.06 100 − 11.82 − 13.61 + 15.73<br />

+ 18.18 + 21.01<br />

+ 30.41 + 32.15<br />

= 192.05<br />

0.04 100 − 11.82 − 13.61 − 15.73<br />

+ 18.18 + 21.01 + 30.41<br />

+ 32.15 + 33.53<br />

= 194.12<br />

0.02 100 − 11.82 − 13.61 − 15.73<br />

− 18.18 + 21.01<br />

+ 30.41 + 32.15<br />

+ 33.53 + 34.26<br />

= 192.02<br />

0 100 − 11.82 − 13.61 − 15.73<br />

− 18.18 − 21.01 + 30.41<br />

+ 32.15 + 33.53<br />

+ 34.26 + 33.90<br />

= 183.90<br />

0.831 32.15<br />

0.557 33.53<br />

0.277 34.26<br />

0 33.90<br />

Although the valve is now closed the waves continue their movement,<br />

and the pressure increments at the valve change sign according to<br />

Fig.12.8. However, as the velocity at the valve is zero and must remain<br />

zero, no new waves can be generated.<br />

B (m 1/2 · s −1 ) Head at valve, h (m) u (m · s −1 ) �h (m)<br />

0 100+11.82−13.61−15.73<br />

− 18.18 − 21.01 − 30.41<br />

+ 32.15 + 33.53<br />

+ 34.26 + 33.90<br />

= 146.72<br />

0 100+11.82+13.61−15.73<br />

− 18.18 − 21.01 − 30.41<br />

− 32.15 + 33.53<br />

+ 34.26 + 33.90<br />

= 109.64<br />

0 100+11.82+13.61+15.73<br />

− 18.18 − 21.01 − 30.41<br />

− 32.15 − 33.53<br />

+ 34.26 + 33.90<br />

= 74.04<br />

0 —<br />

0 —<br />

0 —<br />

0 ...= 41.88 0 —<br />

0 ...= 16.10 0 —<br />

0 ...= 53.28 0 —<br />

Pressure transients 573

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