“…During the past few decades, due to the development of high speed digital computers and numerical methodologies such as Lagrange multiplier technique (Ramkumar et al, 1987), hierarchical finite element method (Bardell, 1991), Kantorovich method (Sakata et al, 1996), finite strip method (Ashour, 2006), methods based on Green functions (Huang et al, 2007), Chebyshev collocation technique (Gupta et al, 2007), quintic splines methods (Lal and Dhanpati, 2007), hybrid method (Kerboua et al, 2007), superposition method (Bhaskar and Sivaram, 2008), boundary knot method (Shi et al, 2009), element-free kp-Ritz method (Zhao et al, 2009), discrete singular convolution method (Civalek et al, 2010), finite cosine integral transform method (Zhong et al, 2014), finite element method (Xiaohui et al, 2011;Houmat, 2012), differential transform method (Semnani et al, 2013), symplectic geometry method (Hu et al, 2012), Ritz method (Eftekhari and Jafari, 2013), unified formulation-cell based smoothed finite element method (Natarajan et al, 2013), local Kriging meshless method (Zhang et al, 2014), etc, a huge amount of work analyzing the dynamic behaviour of plates of various geometries with different boundary conditions has been reported in the literature. In the recent years, differential quadrature (DQ) method introduced by Bellman and Casti (1971) and Bert et al (1988) and its improved versions proposed by Shu and Richards (1992) as generalized differential quadrature (GDQ) method, Striz et al (1995) as harmonic differential quadrature (HDQ) method, Shu and Chew (1997) as Fourier expansionbased differential quadrature (FDQ) method, Liu and Wu (2001) as generalized differential quadrature rule (GDQR), Karami and Malekzadeh (2013) as new differential quadrature (NDQ) method, Krowiak (2006aKrowiak ( , 2006b as spli...…”