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Partial Differential Equations - Modelling and ... - ResearchGate

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Mixed FE Methods on Polyhedral Meshes 31<br />

∫<br />

∫<br />

[− div u − cp]dx=− f dx, k = 1,n. (5)<br />

E k E k<br />

The latter equality results in the discrete equation<br />

∑s k<br />

− u k,i |Γ k,i |−c k |E k |ˆp k = −|E k |f k , (6)<br />

i=1<br />

where<br />

u k,i = 1 ∫<br />

u · n k ds (7)<br />

|Γ k,i | Γ k,i<br />

is the mean value of the normal flux u · n k on Γ k,i ,<br />

c k = 1<br />

|E k |<br />

∫<br />

c dx <strong>and</strong> f k = 1 ∫<br />

f dx (8)<br />

E k<br />

|E k | E k<br />

are the mean values of c <strong>and</strong> f in E k , respectively,<br />

∫<br />

cp dx<br />

ˆp k = ∫ E k<br />

c dx<br />

E k<br />

(9)<br />

is the c-weighted mean value of p in E k . Here, |Γ k,i | <strong>and</strong> |E k | denote the length<br />

of Γ k,i <strong>and</strong> the area of E k , respectively, i = 1,s k ,<strong>and</strong>n k is the outward unit<br />

normal to ∂E k , k = 1,n.<br />

The equation (6) can be written in the matrix form by<br />

B 0,(k)<br />

H ū(k) − c k |E k |ˆp k = −|E k |f k , (10)<br />

where<br />

B 0,(k)<br />

H<br />

= − [ |Γ k,1 | ··· |Γ k,sk | ] ∈ R 1×s k<br />

(11)<br />

<strong>and</strong> ū (k) = [ ] T<br />

u k,1 ,...,u k,sk ∈ R<br />

s k<br />

, k = 1,n. The matrix B 0,(k)<br />

H<br />

will be used<br />

later to derive the final discretization for the problem (4).<br />

The formula (9) assumes that the coefficient c is not equal identically to<br />

zero in E k . In the case c ≡ 0inE k the discrete equation (6) is replaced by<br />

the equation<br />

−<br />

s k<br />

∑<br />

i=1<br />

<strong>and</strong> (10) is replaced by the equation<br />

u k,i |Γ k,i | = −|E k |f k , (12)<br />

B 0,(k)<br />

H ū(k) = −|E k |f k . (13)

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