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2 DGM for elliptic problems

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34 2 Elliptic <strong>problems</strong><br />

∫<br />

〈∇(v − I hp v)〉 · n dS = 0 ∀Γ ∈ F h , v ∈ H 2 (Ω, T h ), (2.146) A7.3<br />

Γ<br />

|I hp v − v| H q (Ω,T h ) ≤ ¯C A h µ−q |v| H µ (Ω,T h ), v ∈ H s (Ω, T h ), h ∈ (0,h (2.147) 0 ), A7.3a<br />

where µ = min(p + 1,s), q = 0,1 and ¯C A is a constant.<br />

Let u ∈ H s (Ω) (s ≥ 1 is an integer) be an exact solution of ptoblem ( 2.1)<br />

A0.1<br />

– ( 2.2). A0.2a Then, in view of ( 2.145) A7.2 and ( 2.146),<br />

A7.3<br />

B h (u − I hp u,v h ) = 0 ∀v h ∈ S h0 , (2.148) A7.4<br />

where S h0 denotes the space of piecewise constant fucntions on T h . Hence, if<br />

Π 0 is the orthogonal projection of L 2 (Ω) onto S h0 , then ( 2.96) A2.41 and ( 2.148)<br />

A7.4<br />

imply that<br />

|B h (u − I hp u,v h )| ≤ ∣ ∣ Bh (u − I hp u,v h − Π 0 v h ) ∣ ∣ +<br />

∣ ∣Bh (u − I hp u,Π 0 v h ) ∣ ∣<br />

≤ C B |||u − I hp u||| |||v h − Π 0 v h ||| ∀v h ∈ S hp . (2.149) A7.5<br />

Obviously,<br />

|u − Π 0 u| H 1 (K) = |u| H 1 (K), K ∈ T h . (2.150) A7.6a<br />

Moreover, it follows from the approximation properties ( 2.34) eq:AP that<br />

‖v − Π 0 v‖ L 2 (K) ≤ C A h K |v| H 1 (K), v ∈ H 1 (K), K ∈ T h . (2.151) A7.6<br />

Let ψ ∈ H 1 (Ω, T h ). Then, using ( eq:MTI 2.19) and ( A3.30 2.120), we find that<br />

|||ψ||| 2 = |ψ| 2 H 1 (Ω,T h ) + Jσ h(ψ,ψ)<br />

∑<br />

(2.152) A7.7<br />

≤ |v| 2 H 1 (Ω,T h ) + 2C W h −1<br />

K ‖ψ‖2 L 2 (∂K)<br />

K∈T h<br />

≤ |ψ| 2 H 1 (Ω,T h ) +2C WC M<br />

∑<br />

K∈T h<br />

(<br />

h −2<br />

K ‖ψ‖2 L 2 (K) + h−1 K ‖ψ‖ L 2 (K)|ψ| H1 (K)<br />

For v ∈ H 1 (Ω, T h ) let us set ψ := v − Π 0 v in ( 2.152). A7.7 Then from ( 2.150) A7.6a –<br />

( 2.151) A7.6 we get<br />

|||v − Π 0 v||| 2 ≤ (1 + 4CAC 2 W C M ) ∑<br />

|v| 2 H 1 (K) (2.153) A7.8<br />

K∈T h<br />

= (1 + 4C 2 AC W C M )|v| 2 H 1 (Ω,T h ) .<br />

On the other hand, if we set ψ := u − I hp u, then by ( 2.152) A7.7 and ( 2.147)<br />

A7.3a<br />

we obtain<br />

)<br />

.<br />

|||u − I hp u||| 2 ≤ ¯C 2 Ah 2µ−2 |u| 2 H µ (Ω + 4 ¯C 2 AC W C M h 2µ−2 |u| 2 H µ (Ω)<br />

= ¯C 2 A(1 + 4C W C M )h 2µ−2 |u| 2 H µ (Ω) .<br />

(2.154) A7.9

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