### Abstract

The finite‐strip method (FSM) is a hybrid technique which combines spectral and finite‐element methods. Finite‐element approximations are made for each mode of a finite Fourier series expansion. The Galerkin formulated method is set apart from other weighted‐residual techniques by the selection of two types of basis functions, a piecewise linear interpolating function and a trigonometric function. The efficiency of the FSM is due in part to the orthogonality of the complex exponential basis: The linear system which results from the weak formulation is decoupled into several smaller systems, each of which may be solved independently. An error analysis for the FSM applied to time‐dependent, parabolic partial differential equations indicates the numerical solution error is O(h^{2} + M^{−r}). M represents the Fourier truncation mode number and h represents the finite‐element grid mesh. The exponent r ≥ 2 increases with the exact solution smoothness in the respective dimension. This error estimate is verified computationally. Extending the result to the finite‐layer method, where a two‐dimensional trigonometric basis is used, the numerical solution error is O(h^{2} + M^{−r} + N^{−q}). The N and q represent the trucation mode number and degree of exact solution smoothness in the additional dimension. © 1993 John Wiley & Sons, Inc.

Original language | English (US) |
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Pages (from-to) | 667-690 |

Number of pages | 24 |

Journal | Numerical Methods for Partial Differential Equations |

Volume | 9 |

Issue number | 6 |

DOIs | |

State | Published - Nov 1993 |

### All Science Journal Classification (ASJC) codes

- Analysis
- Numerical Analysis
- Computational Mathematics
- Applied Mathematics

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## Cite this

*Numerical Methods for Partial Differential Equations*,

*9*(6), 667-690. https://doi.org/10.1002/num.1690090605