# Order of accuracy

In numerical analysis, order of accuracy quantifies the rate of convergence of a numerical approximation of a differential equation to the exact solution. Consider ${\displaystyle u}$, the exact solution to a differential equation in an appropriate normed space ${\displaystyle (V,||\ ||)}$. Consider a numerical approximation ${\displaystyle u_{h}}$, where ${\displaystyle h}$ is a parameter characterizing the approximation, such as the step size in a finite difference scheme or the diameter of the cells in a finite element method. The numerical solution ${\displaystyle u_{h}}$ is said to be ${\displaystyle n}$th-order accurate if the error, ${\displaystyle E(h):=||u-u_{h}||}$ is proportional to the step-size ${\displaystyle h}$ to the ${\displaystyle n}$th power;[1]

${\displaystyle E(h)=||u-u_{h}||\leq Ch^{n}}$

Where the constant ${\displaystyle C}$ is independent of h and usually depends on the solution ${\displaystyle u}$.[2]. Using the big O notation an ${\displaystyle n}$th-order accurate numerical method is notated as

${\displaystyle ||u-u_{h}||=O(h^{n})}$

This definition is strictly depended on the norm used in the space; the choice of such norm is fundamental to estimate the rate of convergence and, in general, all numerical errors correctly.

The size of the error of a first-order accurate approximation is directly proportional to ${\displaystyle h}$. Partial differential equations which vary over both time and space are said to be accurate to order ${\displaystyle n}$ in time and to order ${\displaystyle m}$ in space.[3]

## References

1. LeVeque, Randall J (2006). Finite Difference Methods for Differential Equations. University of Washington. pp. 3–5.
2. Ciarliet, Philippe J (1978). The Finite Element Method for Elliptic Problems. Elsevier. pp. 105–106.
3. Strikwerda, John C (2004). Finite Difference Schemes and Partial Differential Equations (2 ed.). pp. 62–66. ISBN 978-0-898716-39-9.