Condition number

Given a problem ${\displaystyle f}$ and an algorithm ${\displaystyle {\tilde {f}}}$ with an input ${\displaystyle x}$ and output ${\displaystyle {\tilde {f}}(x),}$ the error is ${\displaystyle \delta f(x):=f(x)-{\tilde {f}}(x),}$ the absolute error is ${\displaystyle \|\delta f(x)\|=\left\|f(x)-{\tilde {f}}(x)\right\|}$ and the relative error is ${\displaystyle \|\delta f(x)\|/\|f(x)\|=\left\|f(x)-{\tilde {f}}(x)\right\|/\|f(x)\|.}$

In this context, the absolute condition number of a problem ${\displaystyle f}$ is

${\displaystyle \lim _{\varepsilon \rightarrow 0^{+}}\,\sup _{\|\delta x\|\,\leq \,\varepsilon }{\frac {\|\delta f(x)\|}{\|\delta x\|}}}$

and the relative condition number is

${\displaystyle \lim _{\varepsilon \rightarrow 0^{+}}\,\sup _{\|\delta x\|\,\leq \,\varepsilon }{\frac {\|\delta f(x)\|/\|f(x)\|}{\|\delta x\|/\|x\|}}.}$

For example, the condition number associated with the linear equation Ax = b gives a bound on how inaccurate the solution x will be after approximation. Note that this is before the effects of round-off error are taken into account; conditioning is a property of the matrix, not the algorithm or floating-point accuracy of the computer used to solve the corresponding system. In particular, one should think of the condition number as being (very roughly) the rate at which the solution x will change with respect to a change in b. Thus, if the condition number is large, even a small error in b may cause a large error in x. On the other hand, if the condition number is small, then the error in x will not be much bigger than the error in b.

The condition number is defined more precisely to be the maximum ratio of the relative error in x to the relative error in b.

Let e be the error in b. Assuming that A is a nonsingular matrix, the error in the solution A⁻¹b is A⁻¹e. The ratio of the relative error in the solution to the relative error in b is

${\displaystyle {\frac {\left\|A^{-1}e\right\|}{\left\|A^{-1}b\right\|}}/{\frac {\|e\|}{\|b\|}}={\frac {\left\|A^{-1}e\right\|}{\|e\|}}{\frac {\|b\|}{\left\|A^{-1}b\right\|}}.}$

The maximum value (for nonzero b and e) is then seen to be the product of the two operator norms as follows:

${\displaystyle {\begin{aligned}\max _{e,b\neq 0}\left\{{\frac {\left\|A^{-1}e\right\|}{\|e\|}}{\frac {\|b\|}{\left\|A^{-1}b\right\|}}\right\}&=\max _{e\neq 0}\left\{{\frac {\left\|A^{-1}e\right\|}{\|e\|}}\right\}\,\max _{b\neq 0}\left\{{\frac {\|b\|}{\left\|A^{-1}b\right\|}}\right\}\\&=\max _{e\neq 0}\left\{{\frac {\left\|A^{-1}e\right\|}{\|e\|}}\right\}\,\max _{x\neq 0}\left\{{\frac {\|Ax\|}{\|x\|}}\right\}\\&=\left\|A^{-1}\right\|\,\|A\|.\end{aligned}}}$

The same definition is used for any consistent norm, i.e. one that satisfies

${\displaystyle \kappa (A)=\left\|A^{-1}\right\|\,\left\|A\right\|\geq \left\|A^{-1}A\right\|=1.}$

When the condition number is exactly one (which can only happen if A is a scalar multiple of a linear isometry), then a solution algorithm can find (in principle, meaning if the algorithm introduces no errors of its own) an approximation of the solution whose precision is no worse than that of the data.

However, it does not mean that the algorithm will converge rapidly to this solution, just that it will not diverge arbitrarily because of inaccuracy on the source data (backward error), provided that the forward error introduced by the algorithm does not diverge as well because of accumulating intermediate rounding errors.

The condition number may also be infinite, but this implies that the problem is ill-posed (does not possess a unique, well-defined solution for each choice of data; that is, the matrix is not invertible), and no algorithm can be expected to reliably find a solution.

The definition of the condition number depends on the choice of norm, as can be illustrated by two examples.

If ${\displaystyle \|\cdot \|}$ is the matrix norm induced by the (vector) Euclidean norm (sometimes known as the L² norm and typically denoted as ${\displaystyle \|\cdot \|_{2}}$), then

${\displaystyle \kappa (A)={\frac {\sigma _{\text{max}}(A)}{\sigma _{\text{min}}(A)}},}$

where ${\displaystyle \sigma _{\text{max}}(A)}$ and ${\displaystyle \sigma _{\text{min}}(A)}$ are maximal and minimal singular values of ${\displaystyle A}$ respectively. Hence:

• If ${\displaystyle A}$ is normal, then
  $${\displaystyle \kappa (A)={\frac {\left|\lambda _{\text{max}}(A)\right|}{\left|\lambda _{\text{min}}(A)\right|}},}$$

  
  where ${\displaystyle \lambda _{\text{max}}(A)}$ and ${\displaystyle \lambda _{\text{min}}(A)}$ are maximal and minimal (by moduli) eigenvalues of ${\displaystyle A}$ respectively.
• If ${\displaystyle A}$ is unitary, then ${\displaystyle \kappa (A)=1.}$

The condition number with respect to L² arises so often in numerical linear algebra that it is given a name, the condition number of a matrix.

If ${\displaystyle \|\cdot \|}$ is the matrix norm induced by the ${\displaystyle L^{\infty }}$ (vector) norm and ${\displaystyle A}$ is lower triangular non-singular (i.e. ${\displaystyle a_{ii}\neq 0}$ for all ${\displaystyle i}$), then

${\displaystyle \kappa (A)\geq {\frac {\max _{i}{\big (}|a_{ii}|{\big )}}{\min _{i}{\big (}|a_{ii}|{\big )}}}}$

recalling that the eigenvalues of any triangular matrix are simply the diagonal entries.

The condition number computed with this norm is generally larger than the condition number computed relative to the Euclidean norm, but it can be evaluated more easily (and this is often the only practicably computable condition number, when the problem to solve involves a non-linear algebra, for example when approximating irrational and transcendental functions or numbers with numerical methods).

If the condition number is not significantly larger than one, the matrix is well-conditioned, which means that its inverse can be computed with good accuracy. If the condition number is very large, then the matrix is said to be ill-conditioned. Practically, such a matrix is almost singular, and the computation of its inverse, or solution of a linear system of equations is prone to large numerical errors. A matrix that is not invertible is often said to have a condition number equal to infinity. Alternatively, it can be defined as ${\displaystyle \kappa (A)=\|A\|\|A^{\dagger }\|}$, where ${\displaystyle A^{\dagger }}$ is the Moore-Penrose pseudoinverse. For square matrices, this unfortunately makes the condition number discontinuous, but it is a useful definition for rectangular matrices, which are never invertible but are still used to define systems of equations.

Condition numbers can also be defined for nonlinear functions, and can be computed using calculus. The condition number varies with the point; in some cases one can use the maximum (or supremum) condition number over the domain of the function or domain of the question as an overall condition number, while in other cases the condition number at a particular point is of more interest.

One variable

See also: Significance arithmetic § Transcendental functions

The condition number of a differentiable function ${\displaystyle f}$ in one variable as a function is ${\displaystyle \left|xf'/f\right|}$. Evaluated at a point ${\displaystyle x}$, this is

${\displaystyle \left|{\frac {xf'(x)}{f(x)}}\right|=\left|{\frac {(\log f)'}{(\log x)'}}\right|.}$

Note that this is the absolute value of the elasticity of a function in economics.

Most elegantly, this can be understood as (the absolute value of) the ratio of the logarithmic derivative of ${\displaystyle f}$, which is ${\displaystyle (\log f)'=f'/f}$, and the logarithmic derivative of ${\displaystyle x}$, which is ${\displaystyle (\log x)'=x'/x=1/x}$, yielding a ratio of ${\displaystyle xf'/f}$. This is because the logarithmic derivative is the infinitesimal rate of relative change in a function: it is the derivative ${\displaystyle f'}$ scaled by the value of ${\displaystyle f}$. Note that if a function has a zero at a point, its condition number at the point is infinite, as infinitesimal changes in the input can change the output from zero to positive or negative, yielding a ratio with zero in the denominator, hence infinite relative change.

More directly, given a small change ${\displaystyle \Delta x}$ in ${\displaystyle x}$, the relative change in ${\displaystyle x}$ is ${\displaystyle [(x+\Delta x)-x]/x=(\Delta x)/x}$, while the relative change in ${\displaystyle f(x)}$ is ${\displaystyle [f(x+\Delta x)-f(x)]/f(x)}$. Taking the ratio yields

${\displaystyle {\frac {[f(x+\Delta x)-f(x)]/f(x)}{(\Delta x)/x}}={\frac {x}{f(x)}}{\frac {f(x+\Delta x)-f(x)}{(x+\Delta x)-x}}={\frac {x}{f(x)}}{\frac {f(x+\Delta x)-f(x)}{\Delta x}}.}$

The last term is the difference quotient (the slope of the secant line), and taking the limit yields the derivative.

Condition numbers of common elementary functions are particularly important in computing significant figures and can be computed immediately from the derivative; see significance arithmetic of transcendental functions. A few important ones are given below:

Name	Symbol	Condition number
Addition / subtraction	${\displaystyle x+a}$	${\displaystyle \left|{\frac {x}{x+a}}\right|}$
Scalar multiplication	${\displaystyle ax}$	${\displaystyle 1}$
Division	${\displaystyle 1/x}$	${\displaystyle 1}$
Polynomial	${\displaystyle x^{n}}$	${\displaystyle |n|}$
Exponential function	${\displaystyle e^{x}}$	${\displaystyle |x|}$
Natural logarithm function	${\displaystyle \ln(x)}$	${\displaystyle \left|{\frac {1}{\ln(x)}}\right|}$
Sine function	${\displaystyle \sin(x)}$	${\displaystyle |x\cot(x)|}$
Cosine function	${\displaystyle \cos(x)}$	${\displaystyle |x\tan(x)|}$
Tangent function	${\displaystyle \tan(x)}$	${\displaystyle |x(\tan(x)+\cot(x))|}$
Inverse sine function	${\displaystyle \arcsin(x)}$	${\displaystyle {\frac {x}{{\sqrt {1-x^{2}}}\arcsin(x)}}}$
Inverse cosine function	${\displaystyle \arccos(x)}$	${\displaystyle {\frac {|x|}{{\sqrt {1-x^{2}}}\arccos(x)}}}$
Inverse tangent function	${\displaystyle \arctan(x)}$	${\displaystyle {\frac {x}{(1+x^{2})\arctan(x)}}}$

• Numerical methods for linear least squares
• Hilbert matrix
• Ill-posed problem
• Singular value
• Wilson matrix

• Demmel, James (1990). "Nearest Defective Matrices and the Geometry of Ill-conditioning". In Cox, M. G.; Hammarling, S. (eds.). Reliable Numerical Computation. Oxford: Clarendon Press. pp. 35–55. ISBN 0-19-853564-3.

• Condition Number of a Matrix at Holistic Numerical Methods Institute
• MATLAB library function to determine condition number
• Condition number – Encyclopedia of Mathematics
• Who Invented the Matrix Condition Number? by Nick Higham