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In [[numerical analysis]], '''Richardson extrapolation''' is a [[Series acceleration|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.<ref>{{cite journal
| last=Richardson | first=L. F. | authorlink=Lewis Fry Richardson
| title=The approximate arithmetical solution by finite differences of physical problems including differential equations, with an application to the stresses in a masonry dam
| journal=Philosophical Transactions of the Royal Society A
| year=1911 | volume=210
| issue=459-470 | pages=307–357
| doi=10.1098/rsta.1911.0009
}}</ref><ref>{{cite journal
| last=Richardson | first=L. F. | authorlink=Lewis Fry Richardson
| title=The deferred approach to the limit
| journal=Philosophical Transactions of the Royal Society A
| year=1927 | volume=226
| issue=636-646 | pages=299–349
| doi=10.1098/rsta.1927.0008
| last2=Gaunt
| first2=J. A.
}}</ref>  In the words of [[Garrett Birkhoff|Birkhoff]] and [[Gian-Carlo Rota|Rota]], "... its usefulness for practical computations can hardly be overestimated."<ref>Page 126 of {{cite book | last=Birkhoff | first=Garrett | authorlink=Garrett Birkhoff | coauthors=[[Gian-Carlo Rota]] | title=Ordinary differential equations | publisher=John Wiley and sons | year=1978 | edition=3rd | isbn=0-471-07411-X | oclc= 4379402}}</ref>


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Practical applications of Richardson extrapolation include [[Romberg integration]], which applies Richardson extrapolation to the [[trapezoid rule]], and the [[Bulirsch–Stoer algorithm]] for solving ordinary differential equations.
 
==Example of Richardson extrapolation==
Suppose that we wish to approximate <math>A^*</math>, and we have a method <math>A(h)</math> that depends on a small parameter <math>h</math>, so that
 
<math>A(h) = A^\ast + C h^n + o(h^{n+1})\;</math>
 
Define a new method
 
<math> R(h,k) := \frac{ k^n A(h) - A(kh)}{k^n-1} </math>
 
Then
 
<math> \lim_{h \rightarrow 0 } R(h, k) = \frac{ k^n ( A^* + C h^n + o(h^{n+1}) ) - ( A^* + C k^n h^n + o(h^{n+1}) ) }{ k^n - 1} = A^* + o(h^{n+1}). </math>
 
<math> R(h,k) </math> is called the Richardson [[extrapolation]] of ''A''(''h''), and has a higher-order
error estimate <math> o(h^{n+1}) </math> compared to <math> A(h) </math>.
 
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).
 
==General formula==
Let ''A''(''h'') be an approximation of ''A'' that depends on a positive step size ''h'' with an [[Approximation error|error]] formula of the form
:<math> A - A(h) = a_0h^{k_0} + a_1h^{k_1} + a_2h^{k_2} + \cdots </math>
where the ''a<sub>i</sub>'' are unknown constants and the ''k<sub>i</sub>'' are known constants such that ''h<sup>k<sub>i</sub></sup>'' > ''h<sup>k<sub>i+1</sub></sup>''.
 
The exact value sought can be given by
:<math> A = A(h) + a_0h^{k_0} + a_1h^{k_1} + a_2h^{k_2} + \cdots </math>
which can be simplified with [[Big O notation]] to be
:<math> A = A(h)+ a_0h^{k_0} + O(h^{k_1}).  \,\!</math>
 
Using the step sizes ''h'' and ''h / t'' for some ''t'', the two formulas for ''A'' are:
:<math> A = A(h)+ a_0h^{k_0} + O(h^{k_1})  \,\!</math>
:<math> A = A\!\left(\frac{h}{t}\right) + a_0\left(\frac{h}{t}\right)^{k_0} + O(h^{k_1}) .</math>
 
Multiplying the second equation by ''t''<sup>''k''<sub>0</sub></sup> and subtracting the first equation gives
:<math> (t^{k_0}-1)A = t^{k_0}A\left(\frac{h}{t}\right) - A(h) + O(h^{k_1}) </math>
which can be solved for ''A'' to give
:<math>A = \frac{t^{k_0}A\left(\frac{h}{t}\right) - A(h)}{t^{k_0}-1} + O(h^{k_1}) .</math>
 
By this process, we have achieved a better approximation of ''A'' by subtracting the largest term in the error which was ''O''(''h''<sup>''k''<sub>0</sub></sup>).  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
:<math> A_{i+1}(h) = \frac{t^{k_i}A_i\left(\frac{h}{t}\right) - A_i(h)}{t^{k_i}-1} </math>
such that
:<math> A = A_{i+1}(h) + O(h^{k_{i+1}}) </math>
with <math>A_0=A(h)</math>.
 
The Richardson extrapolation can be considered as a linear [[sequence transformation]].
 
Additionally, the general formula can be used to estimate ''k''<sub>0</sub> 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
:<math>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})</math>
yields an approximate relationship
:<math>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}</math>
which can be solved numerically to estimate ''k''<sub>0</sub>.
 
==Example==
 
Using [[Taylor's theorem]] about h=0,
:<math>f(x+h) = f(x) + f'(x)h + \frac{f''(x)}{2}h^2 + \cdots</math>
the derivative of ''f''(''x'') is given by
:<math>f'(x) = \frac{f(x+h) - f(x)}{h} - \frac{f''(x)}{2}h + \cdots.</math>
 
If the initial approximations of the derivative are chosen to be
:<math>A_0(h) = \frac{f(x+h) - f(x)}{h}</math>
then ''k<sub>i</sub>'' = ''i''+1.
 
For ''t'' = 2, the first formula extrapolated for ''A'' would be
:<math>A = 2A_0\!\left(\frac{h}{2}\right) - A_0(h) + O(h^2) .</math>
 
For the new approximation
:<math>A_1(h) = 2A_0\!\left(\frac{h}{2}\right) - A_0(h) </math>
we can extrapolate again to obtain
:<math> A = \frac{4A_1\!\left(\frac{h}{2}\right) - A_1(h)}{3} + O(h^3) .</math>
 
 
==Example MATLAB code For Richardson Extrapolation==
 
The following demonstrates Richardson extrapolation to help solve the ODE <math>y'(t) = -y^2</math>, <math>y(0) = 1</math> with the Trapezoidal method. In this example we half the step size <math>h</math> each iteration and so in the discussion above we'd have that <math>t = 2</math>. The error of the Trapezoidal method can be expressed in terms of odd powers so that the error over multiple steps can be expressed in even powers and so we take powers of <math>4 = 2^2 = t^2</math> in the pseudocode. We want to find the value of <math>y(5)</math>, which has the exact solution of <math>\frac{1}{5 + 1} = \frac{1}{6} = 0.1666...</math> since the exact solution of the ODE is <math>y(t) = \frac{1}{1 + t}</math>. This pseudocode assumes that a function called <code>Trapezoidal(f, tStart, tEnd, h, y0)</code> exists which performs the trapezoidal method on the function <code>f</code>, with starting point <code>y0</code> and <code>tStart</code>, step size <code>h</code>, and attempts to computes <code>y(tEnd)</code>
 
Starting with too small an initial step size can potentially introduce error into the final solution. Although there are methods designed to help pick the best initial step size, one option is to start with a large step size and then to allow the Richardson extrapolation to reduce the step size each iteration until the error reaches the desired tolerance.  
 
<source lang="matlab">
tStart = 0          %Starting time
tEnd = 5            %Ending time
f = -y^2            %The derivative of y, so y' = f(t, y(t)) = -y^2
                    % The solution to this ODE is y = 1/(1 + t)
y0 = 1              %The initial position (i.e. y0 = y(tStart) = y(0) = 1)
tolerance = 10^-11  %10 digit accuracy is desired
 
maxRows = 20                %Don't allow the iteration to continue indefinitely
initialH = tStart - tEnd    %Pick an initial step size
haveWeFoundSolution = false %Were we able to find the solution to the desired tolerance? not yet.
 
h = initialH
 
%Create a 2D matrix of size maxRows by maxRows to hold the Richardson extrapolates
%Note that this will be a lower triangular matrix and that at most two rows are actually
% needed at any time in the compuation.
A = zeroMatrix(maxRows, maxRows)
 
%Compute the top left element of the matrix
A(1, 1) = Trapezoidal(f, tStart, tEnd, h, y0)
 
%Each row of the matrix requires one call to Trapezoidal
%This loops starts by filling the second row of the matrix, since the first row was computed above
for i = 1 : maxRows - 1 %Starting at i = 1, iterate at most maxRows - 1 times
    h = h/2            %Half the previous value of h since this is the start of a new row
   
    %Call the Trapezoidal function with this new smaller step size
    A(i + 1, 1) = Trapezoidal(f, tStart, tEnd, h, y0)
   
    for j = 1 : i        %Go across the row until the diagonal is reached
        %Use the last value computed (i.e. A(i + 1, j)) and the element from the
        % row above it (i.e. A(i, j)) to compute the next Richardson extrapolate
   
        A(i + 1, j + 1) = ((4^j).*A(i + 1, j) - A(i, j))/(4^j - 1);
    end
   
    %After leaving the above inner loop, the diagonal element of row i + 1 has been computed
    % This diagonal element is the last Richardson extrapolate to be computed 
    %The difference between this extrapolate and the last extrapolate of row i is a good
    % indication of the error
    if(absoluteValue(A(i + 1, i + 1) - A(i, i)) < tolerance)  %If the result is within tolerance
        print("y(5) = ", A(i + 1, i + 1))                      %Display the result of the Richardson extrapolation
        haveWeFoundSolution = true
        break                                                  %Done, so leave the loop
    end
end
 
if(haveWeFoundSolution == false)  %If we weren't able to find a solution to within the desired tolerance
    print("Warning: Not able to find solution to within the desired tolerance of ", tolerance);
    print("The last computed extrapolate was ", A(maxRows, maxRows))
end
</source>
 
==See also==
* [[Aitken's delta-squared process]]
* [[Takebe Kenko]]
 
==References==
<references/>
*''Extrapolation Methods. Theory and Practice'' by C. Brezinski and M. Redivo Zaglia, North-Holland, 1991.
 
==External links==
*[http://math.fullerton.edu/mathews/n2003/RichardsonExtrapMod.html Module for Richardson's Extrapolation], fullerton.edu
*[http://ocw.mit.edu/courses/mathematics/18-304-undergraduate-seminar-in-discrete-mathematics-spring-2006/projects/xtrpltn_liu_xpnd.pdf Fundamental Methods of Numerical Extrapolation With Applications], mit.edu
*[http://www.math.ubc.ca/~feldman/m256/richard.pdf Richardson-Extrapolation]
*[http://www.math.ubc.ca/~israel/m215/rich/rich.html  Richardson extrapolation on a website of Robert Israel (University of British Columbia) ]
 
[[Category:Numerical analysis]]
[[Category:Asymptotic analysis]]

Revision as of 04:32, 2 August 2013

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 trapezoid rule, and the Bulirsch–Stoer algorithm for solving ordinary differential equations.

Example of Richardson extrapolation

Suppose that we wish to approximate , and we have a method that depends on a small parameter , so that

Define a new method

Then

is called the Richardson extrapolation of A(h), and has a higher-order error estimate compared to .

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).

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

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

which can be simplified with Big O notation to be

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

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

which can be solved for A to give

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

such that

with .

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

yields an approximate relationship

which can be solved numerically to estimate k0.

Example

Using Taylor's theorem about h=0,

the derivative of f(x) is given by

If the initial approximations of the derivative are chosen to be

then ki = i+1.

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

For the new approximation

we can extrapolate again to obtain


Example MATLAB code For Richardson Extrapolation

The following demonstrates Richardson extrapolation to help solve the ODE , with the Trapezoidal method. In this example we half the step size each iteration and so in the discussion above we'd have that . The error of the Trapezoidal method can be expressed in terms of odd powers so that the error over multiple steps can be expressed in even powers and so we take powers of in the pseudocode. We want to find the value of , which has the exact solution of since the exact solution of the ODE is . This pseudocode assumes that a function called Trapezoidal(f, tStart, tEnd, h, y0) exists which performs the trapezoidal method on the function f, with starting point y0 and tStart, step size h, and attempts to computes y(tEnd)

Starting with too small an initial step size can potentially introduce error into the final solution. Although there are methods designed to help pick the best initial step size, one option is to start with a large step size and then to allow the Richardson extrapolation to reduce the step size each iteration until the error reaches the desired tolerance.

tStart = 0          %Starting time
tEnd = 5            %Ending time
f = -y^2            %The derivative of y, so y' = f(t, y(t)) = -y^2
                    % The solution to this ODE is y = 1/(1 + t)
y0 = 1              %The initial position (i.e. y0 = y(tStart) = y(0) = 1)
tolerance = 10^-11  %10 digit accuracy is desired

maxRows = 20                %Don't allow the iteration to continue indefinitely
initialH = tStart - tEnd    %Pick an initial step size
haveWeFoundSolution = false %Were we able to find the solution to the desired tolerance? not yet.

h = initialH

%Create a 2D matrix of size maxRows by maxRows to hold the Richardson extrapolates
%Note that this will be a lower triangular matrix and that at most two rows are actually
% needed at any time in the compuation.
A = zeroMatrix(maxRows, maxRows)

%Compute the top left element of the matrix
A(1, 1) = Trapezoidal(f, tStart, tEnd, h, y0)

%Each row of the matrix requires one call to Trapezoidal
%This loops starts by filling the second row of the matrix, since the first row was computed above
for i = 1 : maxRows - 1 %Starting at i = 1, iterate at most maxRows - 1 times
    h = h/2             %Half the previous value of h since this is the start of a new row
    
    %Call the Trapezoidal function with this new smaller step size
    A(i + 1, 1) = Trapezoidal(f, tStart, tEnd, h, y0)
    
    for j = 1 : i         %Go across the row until the diagonal is reached
        %Use the last value computed (i.e. A(i + 1, j)) and the element from the
        % row above it (i.e. A(i, j)) to compute the next Richardson extrapolate
     
        A(i + 1, j + 1) = ((4^j).*A(i + 1, j) - A(i, j))/(4^j - 1);
    end
    
    %After leaving the above inner loop, the diagonal element of row i + 1 has been computed
    % This diagonal element is the last Richardson extrapolate to be computed  
    %The difference between this extrapolate and the last extrapolate of row i is a good
    % indication of the error
    if(absoluteValue(A(i + 1, i + 1) - A(i, i)) < tolerance)   %If the result is within tolerance
        print("y(5) = ", A(i + 1, i + 1))                      %Display the result of the Richardson extrapolation
        haveWeFoundSolution = true
        break                                                  %Done, so leave the loop
    end
end

if(haveWeFoundSolution == false)   %If we weren't able to find a solution to within the desired tolerance
    print("Warning: Not able to find solution to within the desired tolerance of ", tolerance);
    print("The last computed extrapolate was ", A(maxRows, maxRows))
end

See also

References

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  • Extrapolation Methods. Theory and Practice by C. Brezinski and M. Redivo Zaglia, North-Holland, 1991.

External links