“…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.…”