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kinsol

SUNDIALS general-purpose nonlinear system solver

Syntax

[y,val,info,extra] = kinsol(f,y0,options)

Arguments

f

a function, a string or a list, the right hand side of the nonlinear system

y0

a double array: initial guess

options

a sequence of optional named arguments, see the solvers options

y,val

double arrays: approximate solution at the end of solver iterations and value of the system function, at y, respectively

info

an integer, the solver exit code, see the related section below

extra

a MList containing solver information and statistics, see the related section below

Description

kinsol computes the solution of a real or complex system of nonlinear algebraic equations under the classical form

0=F(y)

or under the fixed-point form

y=G(y).

It is an interface to kinsol solver of SUNDIALS library with default inexact Newton method for classical form or fixed-point iterations with Anderson acceleration for fixed-point form. The solver has a specific feature which allows to constrain the sign of solution components (see the options page). Unlike the native implementation, the Scilab interface allows to solve the system when the function and/or solution is complex (see the Complex solutions help page).

In its simplest form, the solver call takes the form

y = kinsol(f,y0)

where y0 is the initial guess, y is the approximate solution yielded by the solver given default tolerance (which can be changed in options). The right hand side can be computed by a Scilab function with one argument, but if you need to pass extra parameters and/or want to use DLL entrypoints see the user functions help page.

Example

In the following example, we solve the following system of equations

\begin{array}{rcl} 2x_1-x_2-\exp(-x_1) &=&0\\ -x_1+2x_2-\exp(-2x_2) &=&0 \end{array}

with the initial guess [0,0], default inexact Newton method and display solver iterations:

function F=fun(x)    
    F = [2*x(1)-x(2)-exp(-x(1))
          -x(1)+2*x(2)-exp(-2*x(2))];
end
x=kinsol(fun, [0 0], display="iter")

PDE example

In the following example, we approximate the solution of the following nonlinear pde

\frac{\partial^2 f}{\partial x^2}+\frac{\partial^2 f}{\partial y^2} = \frac{2}{1+f^2}

with finite differences, on [-1,1]x[-1,1] and a particular nonhomogeneous Dirichlet boundary condition. The band Jacobian is approximated with finite differences.

function out=fun(f, lap, bdy)
    out = lap*f - 2./(1+f.*f)
    out(bdy) = f(bdy)-sign(cos(%pi*(X(bdy)+Y(bdy))));
endfunction

// define square domain [-1,1] x [-1,1]
n = 50;
x=linspace(-1,1,n); y=x;
[X,Y]=meshgrid(x,x);

// build Laplacian operator
dx=x(2)-x(1);
d1x=sparse(ones(n-1,1));
d0x=sparse(ones(n,1));
lap = (diag(d1x,-1)+diag(d1x,1)-2*diag(d0x))/dx/dx;
// use Kronecker product to build matrix of d/dx^2 and d/dy^2
LAP = lap .*. speye(n,n) + speye(n,n) .*. lap;
// Find boundary nodes
BDY = find(X(:)==x(1) | X(:)==x($) | Y(:)==y(1) | Y(:)==y($))';

f = kinsol(list(fun,LAP,BDY),ones(n*n,1), jacBand=[n,n], display="iter");

clf
gcf().color_map=parula(128);
surf(x,x,matrix(f,n,n))

Exit codes

0 Successful function return
1 The initial user-supplied guess already satisfies the stopping criterion
2 The stopping tolerance on scaled step length was satisfied
-5 The linesearch algorithm was unable to find an iterate sufficiently distinct from the current iterate
-6 The maximum number of nonlinear iterations has been reached
-7 Five consecutive steps have been taken that satisfy a scaled step length test
-99 The solver has been stopped by user callback

Extra output and statistics

The extra optional output argument is a MList with fields:

solver

the solver name, "kinsol"

method

the name of the method used by the solver: "Newton" (inexact Newton method), "lineSearch" (inexact Newton method with linesearch globalization), "Picard" (Picard iterations), and "fixedPoint" (fixed-point iterations)

linearSolver

the linear solver used by the method, if applicable. This field is "none" when using fixed-point iterations. In other cases this field can be "dense", "band" or "sparse" depending on the format of the Jacobian provided by the user.

stats

a structure gathering the solver statistics:

nItersthe number of iterations
nRhsEvalsthe number of right hand side evaluations
nRhsEvalsFDthe number of right hand side evaluations that have been used to approximate the Jacobian
nJacEvalsthe number of Jacobian evaluations, when this one has been given by the user
nBacktrackthe number of backtracking steps (lineSearch method)
funcNormThe scaled Euclidian norm of the system function
stepLengththe length of the last step (Newton and lineSearch methods)
etimeelapsed time by the solver

See also

Bibliography

A. C. Hindmarsh, P. N. Brown, K. E. Grant, S. L. Lee, R. Serban, D. E. Shumaker, and C. S. Woodward, "SUNDIALS: Suite of Nonlinear and Differential/Algebraic Equation Solvers," ACM Transactions on Mathematical Software, 31(3), pp. 363-396, 2005. Also available as LLNL technical report UCRL-JP-200037.

Alan C. Hindmarsh and Radu Serban and Cody J. Balos and David J. Gardner and Daniel R. Reynolds and Carol S. Woodward, "User Documentation for kinsol, 2021, v6.1.1, available online at https://sundials.readthedocs.io/en/latest/kinsol

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