“…Predictions of flows using the conventional Navier-Stokes (NS) equations along with different velocity slip and temperature jump conditions at the wall (Arkilic et al, 1997;Karniadakis and Beskok, 2002;Colin, 2005;Karniadakis et al, 2005;Barber and Emerson, 2006;Dongari et al, 2007;Tang et al, 2007a,b;Weng and Chen, 2008;Cao et al, 2009;Chen and Bogy, 2010;Colin, 2012;Zhang et al, 2012b), 2. Modelling of flows employing higher order equations than the conventional NS equations (Hadjiconstantinou, 2000;Jin and Slemrod, 2001;Struchtrup and Torrilhon, 2003;Hadjiconstantinou, 2006;Shan et al, 2006;Ansumali et al, 2007;Lilley and Sader, 2008;Struchtrup and Torrilhon, 2008;Weng and Chen, 2008;Dongari et al, 2009;Roohi and Darbandi, 2009;Dongari et al, 2010), 3. Use of i) kinetic theory of gases (Loyalka, 1971;Cercignani, 1990), ii) Molecular Dynamic (MD) simulations (Bird, 1994;Zhang et al, 2012a), iii) Discrete Simulations Monte Carlo (DSMC) methods (Pan et al, 1999;Hadjiconstantinou, 2000), iv) Non-linear and linearised Boltzmann Equation (BE) (Cercignani, 1975(Cercignani, , 1988Li and Kwok, 2003) and v) Lattice Boltzmann Method (LBM) (Cornubert et al, 1991;Sbragaglia and Succi, 2005;Zheng et al, 2006;…”