Richardson extrapolation

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In numerical analysis, Richardson extrapolation is a sequence acceleration method, used to improve the rate of convergence of a sequence. It is named after Lewis Fry Richardson, who introduced the technique in the early 20th century.[1][2] In the words of Birkhoff and Rota, "... its usefulness for practical computations can hardly be overestimated."[3]

Practical applications of Richardson extrapolation include Romberg integration, which applies Richardson extrapolation to the trapezium rule, and the Bulirsch–Stoer algorithm for solving ordinary differential equations.

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[edit] Example of Richardson extrapolation

Suppose that A(h)\; is an estimation of order h^n\; for A=\lim_{h\to 0}A(h), i.e. A-A(h) = a_n h^n+O(h^m),~a_n\ne0,~m>n. Then

R(h) = A(h/2) + \frac{A(h/2)-A(h)}{2^n-1} = \frac{2^n\,A(h/2)-A(h)}{2^n-1}

is called the Richardson extrapolation of A(h); it is an estimate of order hm for A, with m>n.

More generally, the factor 2 can be replaced by any other factor, as shown below.

Very often, it is much easier to obtain a given precision by using R(h) rather than A(h') with a much smaller h' , which can cause problems due to limited precision (rounding errors) and/or due to the increasing number of calculations needed (see examples below).

[edit] General formula

Let A(h) be an approximation of A that depends on a positive step size h with an error formula of the form

 A - A(h) = a_0h^{k_0} + a_1h^{k_1} + a_2h^{k_2} + \cdots

where the ai are unknown constants and the ki are known constants such that hki > hki+1.

The exact value sought can be given by

 A = A(h) + a_0h^{k_0} + a_1h^{k_1} + a_2h^{k_2} + \cdots

which can be simplified with Big O notation to be

 A = A(h)+ a_0h^{k_0} + O(h^{k_1}).  \,\!

Using the step sizes h and h / t for some t, the two formulas for A are:

 A = A(h)+ a_0h^{k_0} + O(h^{k_1})  \,\!
 A = A\!\left(\frac{h}{t}\right) + a_0\left(\frac{h}{t}\right)^{k_0} + O(h^{k_1}) .

Multiplying the second equation by tk0 and subtracting the first equation gives

 (t^{k_0}-1)A = t^{k_0}A\left(\frac{h}{t}\right) - A(h) + O(h^{k_1})

which can be solved for A to give

A = \frac{t^{k_0}A\left(\frac{h}{t}\right) - A(h)}{t^{k_0}-1} + O(h^{k_1}) .

By this process, we have achieved a better approximation of A by subtracting the largest term in the error which was O(hk0). This process can be repeated to remove more error terms to get even better approximations.

A general recurrence relation can be defined for the approximations by

 A_{i+1}(h) = \frac{t^{k_i}A_i\left(\frac{h}{t}\right) - A_i(h)}{t^{k_i}-1}

such that

 A = A_{i+1}(h) + O(h^{k_{i+1}})

with A0 = A(h).

The Richardson extrapolation can be considered as a linear sequence transformation.

Additionally, the general formula can be used to estimate k0 when neither its value nor A is known a priori. Such a technique can be useful for quantifying an unknown rate of convergence. Given approximations of A from three distinct step sizes h, h / t, and h / s, the exact relationship

A=\frac{t^{k_0}A\left(\frac{h}{t}\right) - A(h)}{t^{k_0}-1} + O(h^{k_1}) = \frac{s^{k_0}A\left(\frac{h}{s}\right) - A(h)}{s^{k_0}-1} + O(h^{k_1})

yields an approximate relationship

A\left(\frac{h}{t}\right) + \frac{A\left(\frac{h}{t}\right) - A(h)}{t^{k_0}-1} \approx A\left(\frac{h}{s}\right) +\frac{A\left(\frac{h}{s}\right) - A(h)}{s^{k_0}-1}

which can be solved numerically to estimate k0.

[edit] Example

Using Taylor's theorem,

f(x+h) = f(x) + f'(x)h + \frac{f''(x)}{2}h^2 + \cdots

the derivative of f(x) is given by

f'(x) = \frac{f(x+h) - f(x)}{h} - \frac{f''(x)}{2}h + \cdots.

If the initial approximations of the derivative are chosen to be

A_0(h) = \frac{f(x+h) - f(x)}{h}

then ki = i+1.

For t = 2, the first formula extrapolated for A would be

A = 2A_0\!\left(\frac{h}{2}\right) - A_0(h) + O(h^2) .

For the new approximation

A_1(h) = 2A_0\!\left(\frac{h}{2}\right) - A_0(h)

we can extrapolate again to obtain

 A = \frac{4A_1\!\left(\frac{h}{2}\right) - A_1(h)}{3} + O(h^3) .

[edit] See also

[edit] References

  1. ^ Richardson, L. F. (1911). "The approximate arithmetical solution by finite differences of physical problems including differential equations, with an application to the stresses in a masonry dam". Philosophical Transactions of the Royal Society of London, Series A 210 (459-470): 307–357. doi:10.1098/rsta.1911.0009. 
  2. ^ Richardson, L. F.; Gaunt, J. A. (1927). "The deferred approach to the limit". Philosophical Transactions of the Royal Society of London, Series A 226 (636-646): 299–349. doi:10.1098/rsta.1927.0008. 
  3. ^ Page 126 of Birkhoff, Garrett; Gian-Carlo Rota (1978). Ordinary differential equations (3rd ed.). John Wiley and sons. ISBN 047107411X. OCLC 4379402. 
  • Extrapolation Methods. Theory and Practice by C. Brezinski and M. Redivo Zaglia, North-Holland, 1991.

[edit] External links

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