2020
DOI: 10.1002/num.22557
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An improvised collocation algorithm with specific end conditions for solving modified Burgers equation

Abstract: In this work, numerical solution of nonlinear modified Burgers equation is obtained using an improvised collocation technique with cubic B-spline as basis functions. In this technique, cubic B-splines are forced to satisfy the interpolatory condition along with some specific end conditions. Crank-Nicolson scheme is used for temporal domain and improvised cubic B-spline collocation method is used for spatial domain discretization. Quasilinearization process is followed to tackle the nonlinear term in the equati… Show more

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Cited by 19 publications
(3 citation statements)
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“…Bratsos et al [30] employed the explicit finite difference scheme to numerically solve the equation.Numerical solution of nonlinear modified Burgers' equation EEJP. 4(2023) is obtained using an improvised collocation technique with cubic B-spline as basis functions in [31]. The authors in [32] provided an orthogonal collocation technique with septic Hermite splines as basis function to obtain the numerical solution of non-linear modified Burgers' equation.…”
Section: Introductionmentioning
confidence: 99%
“…Bratsos et al [30] employed the explicit finite difference scheme to numerically solve the equation.Numerical solution of nonlinear modified Burgers' equation EEJP. 4(2023) is obtained using an improvised collocation technique with cubic B-spline as basis functions in [31]. The authors in [32] provided an orthogonal collocation technique with septic Hermite splines as basis function to obtain the numerical solution of non-linear modified Burgers' equation.…”
Section: Introductionmentioning
confidence: 99%
“…Shallu and V.K. Kukreja [11] obtained a numerical solution to the nonlinear modified Burgers equation using an improvised collocation technique with cubic B-spline as basis functions. In this method, the cubic B-spline is forced to satisfy interpolant conditions with some specific end conditions.…”
Section: Introductionmentioning
confidence: 99%
“…Equation (1) is nonlinear partial differential equation which is applicable in many fields of sciences such as in approximation theory involving wave propagation in viscous fluid [16], heat conduction and continuous stochastic process [8], gas dynamics [34], longitudinal elastic waves in an isotropic solid [42]. Various efforts are taken to obtain the approximate solution of Equation (1) using different numerical schemes such as meshfree quasi‐interpolation scheme [33], variational scheme [1], optimized weighted essentially non‐oscillatory third order scheme [5], quasi‐linear technique [11], weighted average differential quadrature scheme [29], sinc differential quadrature scheme [31], septic B‐spline scheme [45], cubic B‐spline approaches [14, 51], non‐polynomial spline approach [44], hybrid numerical approach [27], quadratic and cubic B‐splines finite element scheme [13, 46], finite difference method [20, 32], finite element scheme [24, 41], automatic differentiation [6], differential quadrature scheme [36, 37], efficient numerical scheme [39], linearized implicit scheme [40], B‐spline Galerkin methods [15], Haar wavelet quasilinearization scheme [26], multiquadratic quasi‐interpolation technique [10], exponential twice continuously differentiable B‐spline scheme [18], quartic B‐spline collocation method [30], implicit and fully implicit exponential finite difference schemes [23], quintic B‐spline collocation scheme [47], combinations of the wavelet and finite volume scheme [38], semi‐implicit finite difference approach [43], modified cubic B‐spline scheme [35], improvised collocation scheme with cubic B‐spline as basis functions [19], radial basis functions with meshfree algorithms [28], two meshfree approaches [48], cubic trigonometric B‐spline approach [50], meshless technique by applying Lie group integrator with multiquadric radial basis functions [49], MIEELDLD technique [4], and so on.…”
Section: Introductionmentioning
confidence: 99%