Error estimates of the cubic interpolated pseudo-particle scheme for one-dimensional advection equations

Error estimates of cubic interpolated pseudo-particle scheme (CIP scheme) for the one-dimensional advection equation with periodic boundary conditions are presented. The CIP scheme is a semi-Lagrangian method involving the piecewise cubic Hermite interpolation. Although it is numerically known that the space-time accuracy of the scheme is third order, its rigorous proof remains an open problem. In this paper, denoting the spatial and temporal mesh sizes by h and $$\Delta t$$ respectively, we prove an error estimate $$O(\Delta t^3 + \frac{h^4}{\Delta t})$$ in $$L^2$$ -norm theoretically, which justifies the above-mentioned prediction if $$h = O(\Delta t)$$ . We also derive error bounds in the $$H^1$$ - and $$H^2$$ -norms. The proof is based on properties of the interpolation operator; the most important one is that it behaves as the $$L^2$$ projection for the second-order derivatives. We remark that the same strategy perfectly works as well to address an error estimate for the semi-Lagrangian method with the cubic spline interpolation.

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Publication Details

Journal
Japan Journal of Industrial and Applied Mathematics
Published
2026-02-01
DOI
https://doi.org/10.1007/s13160-025-00750-1
Primary Topic
Fluid Dynamics Simulations and Interactions
Type
article
Field-Weighted Citation Impact
0.00

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article

Error estimates of the cubic interpolated pseudo-particle scheme for one-dimensional advection equations

Takahito Kashiwabara, Haruki Takemura
Japan Journal of Industrial and Applied Mathematics
Fluid Dynamics Simulations and Interactions
article

Error estimates of the cubic interpolated pseudo-particle scheme for one-dimensional advection equations

Takahito Kashiwabara, Haruki Takemura
article en

Abstract

Error estimates of cubic interpolated pseudo-particle scheme (CIP scheme) for the one-dimensional advection equation with periodic boundary conditions are presented. The CIP scheme is a semi-Lagrangian method involving the piecewise cubic Hermite interpolation. Although it is numerically known that the space-time accuracy of the scheme is third order, its rigorous proof remains an open problem. In this paper, denoting the spatial and temporal mesh sizes by h and $$\Delta t$$ respectively, we prove an error estimate $$O(\Delta t^3 + \frac{h^4}{\Delta t})$$ in $$L^2$$ -norm theoretically, which justifies the above-mentioned prediction if $$h = O(\Delta t)$$ . We also derive error bounds in the $$H^1$$ - and $$H^2$$ -norms. The proof is based on properties of the interpolation operator; the most important one is that it behaves as the $$L^2$$ projection for the second-order derivatives. We remark that the same strategy perfectly works as well to address an error estimate for the semi-Lagrangian method with the cubic spline interpolation.

Japan Journal of Industrial and Applied MathematicsVol. 43(1)
The University of Tokyo (JP)
Japan Society for the Promotion of Science
Openalex Percentile: Top 67%
Fluid Dynamics Simulations and Interactions
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