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Download full text - ELSA - Europa

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Treatment of momentum equation<br />

• Previous integral statement is unable to furnish enough<br />

equations, since the velocity field in each element depends<br />

upon Nd parameters (N being the number of nodes and d the<br />

space dimension).<br />

• One formulates a variational statement associated with the<br />

differential form of the momentum equation expressed in<br />

mixed coordinates.<br />

• Final result is principle of virtual power (corresponding to<br />

principle of virtual displacements in solid mechanics).<br />

13<br />

Treatment of momentum equation (2)<br />

• The principle of virtual power reads:<br />

∂v<br />

∂( δ v )<br />

δv ρ dV = δv ρ( w −v)<br />

⋅∇ v dV + δv ρg dV + p dV + δv T dS<br />

∫ ∫ ∫ ∫ ∫<br />

i<br />

i<br />

i i i i i i i<br />

∂t<br />

∂x<br />

V() t V() t V() t V() t i<br />

S()<br />

t<br />

vi<br />

are the components of fluid velocity v<br />

δ v i<br />

g i<br />

are arbitrary admissible variations of the fluid velocity<br />

are the components of the acceleration of gravity<br />

T i<br />

are the component of prescribed boundary loads per unit area<br />

x i<br />

are spatial coordinates (current position of particles in fixed frame)<br />

14<br />

7

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