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Sirgue, Laurent, 2003. Inversion de la forme d'onde dans le ...

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2.2. INVERSION OF LINEAR PROBLEMS 29<br />

2.2.2.5 The conjugate gradient method<br />

Whi<strong>le</strong> the steepest <strong>de</strong>scent method assures that the convergence will be reached in a finite number<br />

of iterations, conjugate gradient method improve the convergence rate at litt<strong>le</strong> additional<br />

cost. The conjugate gradient optimises the mo<strong>de</strong>l space search by avoiding to update the mo<strong>de</strong>l<br />

in a direction that has already been searched. The current update direction ∇ m E is then the<br />

conjugate of the previous update direction. The inversion process is thus assured to converge in<br />

n m iterations, where n m is the number of mo<strong>de</strong>l parameter. The conjugate gradient is <strong>de</strong>fined<br />

as (Po<strong>la</strong>k and Ribière, 1969)<br />

(<br />

∇m E (k) − ∇<br />

∇ m E (k) = ∇ m E (k) m E (k−1)) ∇ m E (k)<br />

+<br />

∇<br />

∇ m E (k−1)t ∇ m E (k−1) m E (k−1) . (2.53)<br />

From equation (2.53), we can see that conjugate gradient belongs to the family of gradient<br />

preconditioning that add a vector to the steepest ascent direction as <strong>de</strong>scribed in the previous<br />

section.<br />

2.2.2.6 Numerical examp<strong>le</strong>s<br />

In or<strong>de</strong>r to illustrate the resolution of linear system using local techniques, I chose as an examp<strong>le</strong>,<br />

the linear system of 2 equations and 2 unknowns <strong>de</strong>fined as<br />

⎧<br />

⎨<br />

⎩<br />

m 1 + m 2 = 2<br />

−2m 1 + 3m 2 = 1 . (2.54)<br />

The solution of (2.54) is equiva<strong>le</strong>nt to finding the intersection of the 2 straight lines as shown<br />

Figure 2.6a). The solution is evi<strong>de</strong>nt as the straight lines intersect in m true<br />

forward prob<strong>le</strong>m can be expressed in algebraic form using equation (2.4) with<br />

⎛<br />

G = ⎝ 1 1<br />

⎞<br />

⎛<br />

⎠ , m = ⎝ m ⎞<br />

⎛<br />

1<br />

⎠ , d obs = ⎝ 2 ⎞<br />

⎠ .<br />

−2 3<br />

m 2 1<br />

The corresponding misfit function expressed with respect to the component of m is<br />

E = 5m 2 1 + 10m2 2 − 10m 1m 2 − 10m 2 + 5<br />

= (1, 1). The<br />

A SVD of G was carried out using the subroutine svdcmp (Press et al., 1992), yielding the<br />

eigenvectors and singu<strong>la</strong>r values<br />

⎛<br />

⎞ ⎛<br />

0.996 0.09<br />

U ≃ ⎝ ⎠ , Λ ≃ ⎝ 1.382 0<br />

⎞<br />

⎠ ,<br />

−0.09 0.996<br />

0 3.618<br />

⎛<br />

⎞<br />

0.851 −0.526<br />

V ≃ ⎝ ⎠ .<br />

0.526 0.851

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