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Waterhammer with fluid-structure interaction

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Abstract

The classical theory of waterhammer is a well-known and accepted basis for the prediction of pressure surges in piping systems. In this theory the piping system is assumed not to move. In practice however piping systems move when they are loaded by severe pressure surges, which for instance occur after rapid valve closure or pump failure. The motion of the piping system induces pressure surges which are not taken into account in the classical theory.

In this article the interaction between pressure surges and pipe motion is investigated. Three interaction mechanisms are distinguished: friction, Poisson and junction coupling. Numerical experiments on a single straight pipe and a liquid loading line show that interaction highly influences the extreme pressures during waterhammer occurrences.

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Abbreviations

A f :

cross-sectional discharge area

A t :

cross-sectional pipe wall area

c f :

pressure wave speed in fluid

c t :

axial stress wave speed in pipe wall

E :

Young's modulus for pipe wall material

e :

pipe wall thickness

f :

Darch-Weisbach friction coefficient

g :

gravitational acceleration

H :

fluid pressure head

h :

elevation of pipe

K f :

fluid bulk modulus

P :

fluid pressure

R :

internal radius of pipe

T c :

valve closure time

t :

time

u r :

radial displacement of pipe

u z :

axial displacement of pipe

u z :

axial velocity of pipe

V :

fluid velocity

z :

distance along pipe

γ :

elevation angle of pipe

λ :

length of pressure wave

ν :

Poisson's ratio

ρ f :

fluid density

ρ t :

density of pipe wall material

z :

axial pipe stress

σϕ :

hoop stress

References

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Tijsseling, A.S., Lavooij, C.S.W. Waterhammer with fluid-structure interaction. Appl. sci. Res. 47, 273–285 (1990). https://doi.org/10.1007/BF00418055

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  • DOI: https://doi.org/10.1007/BF00418055

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