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Untitled - Cdm.unimo.it

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192 Polynomial Approximation of Differential Equations<br />

Then, there exists a unique solution U ∈ X of problem<br />

(9.3.8) B(U,φ) = F(φ), ∀φ ∈ X.<br />

Moreover, we can find a pos<strong>it</strong>ive constant C4 > 0 such that<br />

(9.3.9) UX ≤ C4 sup<br />

φ∈X<br />

φ≡0<br />

|F(φ)|<br />

.<br />

φX<br />

The Lax-Milgram theorem is a powerful tool for proving existence and uniqueness for a<br />

large class of linear differential problems. Though the proof is not difficult, we om<strong>it</strong> <strong>it</strong><br />

for simplic<strong>it</strong>y. Applications and extensions have been considered in many publications.<br />

We suggest the following authors: lax and milgram(1954), brezis(1983), brezzi and<br />

gilardi(1987). Inequal<strong>it</strong>y (9.3.6) plays a fundamental role in the proof of theorem<br />

9.3.1. It is in general known as a coerciveness cond<strong>it</strong>ion and indicates that (9.3.8) is an<br />

elliptic problem.<br />

The final step is to check wether the Lax-Milgram theorem can be applied to study<br />

the solution of (9.3.4). It is qu<strong>it</strong>e easy to show that X ≡ H1 0,w(I) ⊂ C0 ( Ī) is a Hilbert<br />

space (see section 5.3). In add<strong>it</strong>ion, inequal<strong>it</strong>ies (9.3.5), (9.3.6) and (9.3.7) are directly<br />

obtained from the following result (we recall that the norm in H 1 0,w(I) is given by<br />

(5.7.7)).<br />

Theorem 9.3.2 - Let ν := α = β w<strong>it</strong>h −1 < ν < 1. Then, we can find three pos<strong>it</strong>ive<br />

constants C1,C2,C3 such that<br />

<br />

<br />

(9.3.10) <br />

ψ ′ (φw) ′ <br />

<br />

dx<br />

≤ C1<br />

(9.3.11)<br />

(9.3.12)<br />

I<br />

<br />

<br />

<br />

<br />

I<br />

<br />

[ψ<br />

I<br />

′ ] 2 w dx<br />

ψ<br />

I<br />

′ (ψw) ′ dx ≥ C2<br />

<br />

<br />

fφw dx<br />

≤ C3 f L 2 w (I)<br />

<br />

I<br />

1<br />

2 <br />

I<br />

[φ ′ ] 2 1<br />

w dx<br />

2<br />

, ∀ψ,φ ∈ H 1 0,w(I),<br />

[ψ ′ ] 2 w dx, ∀ψ ∈ H 1 0,w(I),<br />

<br />

[φ<br />

I<br />

′ ] 2 w dx<br />

1<br />

2<br />

, ∀φ ∈ H 1 0,w(I).

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