“…To seek the exact solutions of the nonlinear partial differential equations, many methods have been proposed, for instance the inverse scattering transformation (IST) (Ablowitz & Segur, 2000), B€ acklund transformation (Rogers & Schief, 2002), Painlev e analysis method (Chowdhury, 1999), Darboux transformation (DT) (Gu, Hu, & Zhou, 2005), Hirota direct method (Hirota, 2004), the tanh-function method (Parkes & Duffy, 1996;Zhang, Xu, & Li, 2002), the improved F-expansion method (Islam, Khan, Akbar, & Mastroberardino, 2014;Wang & Zhang, 2005), the modified simple equation method (Akter & Akbar, 2015;Khan, Akbar, & Alam, 2013), the (G 0 =G)-expansion and extend (G 0 =G)-expansion method (Akbar & Ali, 2011;Akbar, Ali, & Mohyud-Din, 2013;Alam, Hafez, Belgacem, & Akbar, 2015b;Zayed & Shorog, 2010), the Exp-function method (He & Abdou, 2007;, the generalized Kudryashov method (Khan & Akbar, 2016), the expðÀUðgÞÞ-expansion and expðUðgÞÞ method (Alam, Hafez, Akbar, & Roshid, 2015a;Roshid & Rahman, 2014), the extended three-wave method Li, Dai, & Liu, 2011;Singh & Gupta, 2016;Wang, Dai, & Liang, 2010). In this paper, based on the bilinear form, we consider exact solutions including solitary wave solution, periodic solitary solution and rational solution of the classical Boussinesq (CB) system (see Wu & Zhang, 1996) …”