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Exact(13)
Given the iterative origin, then the set of the n th iteration is obtained by (14).
Then the next iteration is obtained as the projection of the current iterate onto the intersection of the feasible set with the convex set and the half-space containing the solution set.
Weak convergence of the purposed iteration is obtained in a Banach space.
The accuracy constraint for the next iteration is obtained by solving.
Halpern's iteration is obtained by replacing and in (3.1) by using the formalism of Hilbert spaces, for all (see, e.g., [4, 9, 10]).
Consequently, the LM step size Δ at each iteration is obtained by solving: J T J + h I Δ = J T f, (16).
Similar(47)
However, after the results of the first iteration were obtained, the equivalent damping was changed in the next iterations to improve the substitute structure/time-history agreement.
Parameter sets for the next iteration were obtained by randomly selecting Xa or Xa' for each virtual sample.
Thus, an upper bound on the total number of iterations is obtained by multiplying the number of outer iterations and the number of inner iterations.
For the λ k i = 1, unrelaxed parameter, the POCS estimate after k iterations is obtained as z i k = P D i j ( k ) P D i j ( k - 1 )... P D i j ( 0 ) z i 0. (9).
A significant speedup and reduction in the number of iterations are obtained when compared to the standard basis.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com