2018 IEEE International Symposium on Antennas and Propagation &Amp; USNC/URSI National Radio Science Meeting 2018
DOI: 10.1109/apusncursinrsm.2018.8608706
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An Explicit Marching-on-in-time Scheme for Solving the Kirchhoff Integral Equation

Abstract: An explicit marching-on-in-time scheme for solving the Kirchhoff integral equation enforced on an acoustically rigid scatterer is proposed. The unknown velocity potential introduced on the surface of scatterer is expanded using unit pulse functions in space and Lagrange polynomial interpolation functions in time. The resulting system is cast in the form of an ordinary differential equation and then integrated numerically in time using a predictor-corrector scheme to obtain the unknown expansion coefficients. N… Show more

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Cited by 3 publications
(3 citation statements)
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“…The predictor and corrector coefficient vectors, p and c are obtained using the sixthorder Adams-Bashforth and backward difference formulas [50], respectively. The convergence threshold for the corrector updates [(CE) m ] is set to PECE = 10 −13 [see (54)]. The matrix equations in ( 43), ( 46), (50), and ( 53) are iteratively solved using the transpose-free quasi-minimal residual (TFQMR) method [67].…”
Section: Numerical Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…The predictor and corrector coefficient vectors, p and c are obtained using the sixthorder Adams-Bashforth and backward difference formulas [50], respectively. The convergence threshold for the corrector updates [(CE) m ] is set to PECE = 10 −13 [see (54)]. The matrix equations in ( 43), ( 46), (50), and ( 53) are iteratively solved using the transpose-free quasi-minimal residual (TFQMR) method [67].…”
Section: Numerical Resultsmentioning
confidence: 99%
“…Inserting these expansions into TD-EFVIE and testing the resulting equation using SWG functions yield a system of ordinary differential equations (ODEs) in timedependent expansion coefficients of the SWG basis functions. A P E(CE) m scheme is used to integrate this system of ODEs in time for the unknown electric field expansion coefficients [38,39,43,[47][48][49][50][51][52][53][54][55][56][57]. Similarly, expansions of the electric field and the electric flux are inserted into the nonlinear constitutive relation and its "inverse" obtained using the Padé approximant [58][59][60].…”
Section: Introductionmentioning
confidence: 99%
“…It should be noted here that TDCPIE is obtained by linearly combining TDPIE with its normal derivative. Coupling parameters of this combination are carefully selected to enable the computation of the singular integrals that appear in the expressions of the matrix elements resulting from the Nyström discretization in space [28][29][30][31][32][33][34][35][36][37][38][39][40].…”
Section: Introductionmentioning
confidence: 99%