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Thread: Implementation of psuedo-arclength continuation

  1. #1
    Jul 2009

    Question Implementation of psuedo-arclength continuation

    Hi there,

    I have a quick question regarding pseudo-arclength continuation. As some background, I am a chemical engineer, not a mathematician, applied or otherwise, so my knowledge of numerical methods is limited to the "standard" stuff.

    I've been reading up as extensively as I can on pseudo-arclength continuation, but unfortunately, it's all from second-hand sources; I don't have access to Keller's original paper. Here's what I understand at this point:

    We want to solve a problem $\displaystyle F(x,\lambda)=0$. We assume that the solution is known at $\displaystyle x^0$ and $\displaystyle \lambda^0$. To avoid the singularity of the Jacobian, and therefore the breakdown of Newton's method, at turning points, $\displaystyle x$ and $\displaystyle \lambda$ both become parameterised by arclength ($\displaystyle s$), and we end up with an augmented system of equations to solve:

    $\displaystyle F(x,\lambda)=0$
    $\displaystyle \left(u-u^{0}\right)\mathrm{d}u^{0}/\mathrm{d}s+\left(\lambda-\lambda^{0}\right)\mathrm{d}\lambda^{0}/\mathrm{d}s-\Delta S=0$

    While this seems simple enough, how does one obtain the derivatives w.r.t $\displaystyle s$? Not a single text seems to mention this. Ideas that spring to mind are forward differences using, say, cubic splines; however, that seems horrendously inefficient to me. There must be a better way!

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  2. #2
    Jul 2009

    Re: Implementation of psuedo-arclength continuation

    I found the answer: a procedure is described in Kubicek's Algorithm 502 in ACM Trans. Math. Software.
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