Titlebook: Viscometric Flows of Non-Newtonian Fluids; Theory and Experimen Bernard D. Coleman,Hershel Markovitz,Walter Noll Book 1966 Springer-Verlag

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Theory of Incompressible Simple Fluids,r position in space. Let . be the position in Euclidean space . of the material point . at time ., which we interpret as the present time. Suppose that at time ., say . ≤ ., this same material point . occupied the position . in .. For the dependence of . on ., .,and ., we write

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Introduction,1) into the dynamical equations are called the .. Equation (1.2) expresses the assumption of incompressibility, i.e., constancy of mass density. More precise explanations of (1.1) and (1.2) will be given in the text.

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0081-3877 se that theory to discuss the design and interpretation of ex­ periments. We are able to present the theory with less mathematical machinery than was used in our original papers, partly because this Tract has more limited aims than those papers, and partly because we employ a method, found by Noll a

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Introduction,ensor, . is the stress tensor, . is a pressure, and . is the viscosity, a material constant. The field equations which result from substitution of (1.1) into the dynamical equations are called the .. Equation (1.2) expresses the assumption of incompressibility, i.e., constancy of mass density. More

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Theory of Incompressible Simple Fluids,r position in space. Let . be the position in Euclidean space . of the material point . at time ., which we interpret as the present time. Suppose that at time ., say . ≤ ., this same material point . occupied the position . in .. For the dependence of . on ., .,and ., we write

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Experimental Methods and Results, chapter these material functions were related to measurable quantities such as velocities, volume discharges per unit time, angular velocities, applied forces and torques, differences of normal thrusts, etc. Without attempting an exhaustive summary, we here discuss practical methods of determining