Time derivative of 2mD reduced dynamics

Contents

function J = ode_2mDSSM_cartesian_DFDP(z, p, data)
        

ODE_2MDSSM_POLAR_DFDX

This function presents vectorized implementation of the Jacobian of the vector field of the reduced dynamics on 2m-dimensional SSMs with respect to system parameters p. Here z is a 2m-dimensinoal state vector and p is parameter vector for excitation frequency and amplitude. All other info such as eigenvalues of master subspace, coefficients of nonlinear terms is included in the structure data. The state vector here is in the form of polar coordinate.

See also: ODE_2MDSSM_POLAR_DFDX

% extract data fields
mFreqs = data.mFreqs;
mFreqs = mFreqs(:);
iNonauto = data.iNonauto;
rNonauto = data.rNonauto;

% rename state and parameter
zRe = z(1:2:end-1,:);
zIm = z(2:2:end,:);
om  = p(1,:);
epsf= p(2,:);
nt  = numel(om);

J = zeros(size(z,1),2,nt);

% w.r.t. Omega
J(1:2:end-1,1,:) = mFreqs.*zIm;
J(2:2:end,1,:)   = -mFreqs.*zRe;
% w.r.t. epsilon
% nonautonomous leading part
m = numel(mFreqs);
yRe = zeros(m,nt);
yIm = zeros(m,nt);
for i=1:numel(iNonauto)
    id = iNonauto(i);
    r  = rNonauto(i);
    rRe = real(r);
    rIm = imag(r);
    yRe(id,:) = yRe(id,:)+rRe;
    yIm(id,:) = yIm(id,:)+rIm;
end
J(1:2:end-1,2,:) = yRe;
J(2:2:end,2,:)   = yIm;

if data.isbaseForce
    J(1:2:end-1,1,:) = J(1:2:end-1,1,:)+reshape(2*epsf.*om.*yRe,[m,1,nt]);
    J(2:2:end,1,:)   = J(2:2:end,1,:)+reshape(2*epsf.*om.*yIm,[m,1,nt]);
    J(1:2:end-1,2,:) = J(1:2:end-1,2,:).*reshape(repmat(om.^2,[m,1]),[m,1,nt]);
    J(2:2:end,2,:)   = J(2:2:end,2,:).*reshape(repmat(om.^2,[m,1]),[m,1,nt]);
end

% func = @(z,p) ode_2mDSSM_cartesian(z,p,data);
% JJ = coco_ezDFDP('f(x,p)v',func,z,p);
% ers = max(abs(J(:)-JJ(:)))
        

end
        

Published with MATLAB® R2023a