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Zero stability

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Zero-stability, also known as D-stability in honor of Germund Dahlquist,[1] refers to the stability of a numerical scheme applied to the simple initial value problem {\displaystyle y'(x)=0}.

A linear multistep method is zero-stable if all roots of the characteristic equation that arises on applying the method to {\displaystyle y'(x)=0} have magnitude less than or equal to unity, and that all roots with unit magnitude are simple.[2] This is called the root condition[3] and means that the parasitic solutions of the recurrence relation will not grow exponentially.

Example#edit

The following third-order method has the highest order possible for any explicit two-step method[2] for solving {\displaystyle y'(x)=f(x)}: {\displaystyle y_{n+2}+4y_{n+1}-5y_{n}=h(4f_{n+1}+2f_{n}).} If {\displaystyle f(x)=0} identically, this gives a linear recurrence relation with characteristic equation {\displaystyle r^{2}+4r-5=(r-1)(r+5)=0.} The roots of this equation are {\displaystyle r=1} and {\displaystyle r=-5} and so the general solution to the recurrence relation is {\displaystyle y_{n}=c_{1}\cdot 1^{n}+c_{2}(-5)^{n. Rounding errors in the computation of {\displaystyle y_{1 would mean a nonzero (though small) value of {\displaystyle c_{2 so that eventually the parasitic solution {\displaystyle (-5)^{n would dominate. Therefore, this method is not zero-stable.

References#edit

  1. ^ Dahlquist, Germund (1956). "Convergence and stability in the numerical integration of ordinary differential equations". Mathematica Scandinavica. 4 (4): 33–53. doi:10.7146/math.scand.a-10454. JSTOR 24490010.
  2. ^ a b Hairer, Ernst; Nørsett, Syvert; Wanner, Gerhard (1987). Solving Ordinary Differential Equations I. Berlin: Springer-Verlag. pp. 326–328.
  3. ^ Butcher, John C (1987). The Numerical Analysis of Ordinary Differential Equations. Wiley. p. 11.

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