“…Rivlin and Ericksen, and Coleman and Noll have presented constitutive relations for the stress tensor as a function of the symmetric part of the velocity gradient and its higher (total) derivatives. Amongst the many models, the Coleman-Noll constitute equation: T ¼ ÀpI þ lA 1 þ a 1 A 2 þ a 2 A 2 1 , which is based on the postulate of gradually fading memory for an incompressible second -order fluid, has received special attention [13][14][15][16][17][18][19][20][21][22][23][24][25][26][27][28][29][30]. Here T is the stress tensor, p is the pressure, I is the unit matrix, l, a 1 , a 2 , are material constants with a 1 < 0, and A 1 and A 2 are the Rivlin-Ericksen tensors defined by:…”