“…Substituting 1 , 1 T and T 2 into Eqs (3.13)-(3.14), we can obtain expressions for R 31 , R 32 easily. Now by applying the solvability condition for the existence of third order solution, we get the Ginzburg-Landau equation (Bhaduria and Kiran [39,40,54], Kiran [41,42,45,61], Keshri et al [44], Manjula et al [47],) for stationary convection with time-periodic coefficients in the form…”