An unconditionally stable alternating direction implicit scheme for the two space dimensional linear hyperbolic equation
By Ranjan Kumar Mohanty, M. Jain, P. Mohanty. 2001
122 citations recorded by the source corpus.
Subfields: Applied Mathematics, Numerical Analysis
View Paper: https://www.semanticscholar.org/paper/35f88dd43734b27e06cfafdfa912f52e6edc0221
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Applied Mathematics
- Ali Shokri
- Arezou Ghesmati
- Mehdi Dehghan
- M. Tatari
- Mehrdad Lakestani
- S. Yousefi
- Abbas Saadatmandi
- Mohsen Razzaghi
In Numerical Analysis
- Ali Shokri
- Arezou Ghesmati
- Mehdi Dehghan
- Mehrdad Lakestani
- Ali Lotfi
- S. Yousefi
- Abbas Saadatmandi
- Elyas Shivanian
Citations in the corpus
- Solution of the second-order one-dimensional hyperbolic telegraph equation by using the dual reciprocity boundary integral equation (DRBIE) method (2010, methodology): “In [24] a three-level implicit unconditionally stable alternating direction implicit (ADI) method for the two-dimensional linear hyperbolic equations is presented, which its accuracy is second order for both time and space components.”
- High order implicit collocation method for the solution of two‐dimensional linear hyperbolic equation (2009, unknown): “Mohanty and Jain [1] introduced a new unconditionally stable alternating direction implicit (ADI) scheme of second order accurate in both spatial and time components for the partial differential equation (1.”
- A numerical method for solving the hyperbolic telegraph equation (2008, background): “[5, 6] developed new three-level implicit unconditionally stable alternating direction implicit schemes for the two and three-space-dimensional linear hyperbolic equations.”