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Homework 3

CM3110 Transport Processes I

Dr. F. A. Morrison

  1. Geankoplis 3rd edition 2.10-1.  Viscosity may be determined for a liquid by subjecting it to Poiseuille flow in a tube.  In a horizontal tube of length 0.1585m and of diameter 2.222mm a fluid is made to flow under a pressure drop of 131 mm water.  The flow rate under these conditions at steady state is 5.33 X 10-7 m3/s.  The density of the fluid is 912 kg/m3 and the density of water is 996 kg/m3. Calculate the viscosity of the fluid; give your answer in Pa s. SOLUTION
  2. Using the microscopic momentum balance, calculate the velocity profile and shear stress profile for steady Poiseuille flow in a tube.  The problem is the same as that which we solved in class using shell balances.  The solution is the same as that which we obtained using shell balances.
  3. Using the microscopic momentum balance, calculate the velocity profile and shear stress profile for steady state flow of an incompressible, power-law fluid down an inclined plane (similar to the problem we did in class but this time with the power-law equation instead of Newton's law of viscosity). Use the same coordinate system as we did in class. You may assume the flow is well developed, and you may neglect edge effects. The inclined plane makes an angle b with gravity. SOLUTION
  4. Calculate the steady state velocity profile and shear stress profile for the flow of an incompressible, Newtonian fluid between two concentric cylinders when both cylinders are rotating.  The radius of the inner cylinder is R1, and it is moving with an angular velocity of w1.  The radius of the outer cylinder is R2, and it is moving with an angular velocity of w2.  The cylinders are long, and we can therefore neglect the effects of the open top and of the bottom on the flow. SOLUTION
  5. In class I showed the plots of the solution for Poiseuille flow (pressure-driven flow) in a tube of a power-law fluid.  The complete solution is:.
    1. Non-dimensionalize this equation, i.e., cast it in the form .
    2. Using a computer (for example, Excel, Matlab, Mathematica), plot the non-dimensional velocity function versus the non-dimensional radius for n=1, 0.8, 0.6, 0.4, and 0.2.
    3. What is the effect of the power-law index, n, on the shape of the non-dimensional velocity?
    4. What is the solution for vz(r) when n=0? SOLUTION
  6. Geankoplis 3rd edition 2.5-1 Whole milk at 293K having a density of 1030 kg/m3 and viscosity of 2.12 cp is flowing at the rate of 0.605 kg/s in a glass pipe having a diameter of 63.5 mm.  a)  What is the Re number for this flow?  Is the flow laminar or turbulent?  b)  Calculate the flow rate and average velocity needed for a Reynolds number of 2100. SOLUTION
  7. HONORS Problem: The equations of motion (components of the vector differential momentum balance equation) in terms of stresses (txy, txx, txz, etc.) are useful in dimensional analysis of the behavior of non-Newtonian fluids. Show for the power-law, non-Newtonian fluid that the dimensionless groups obtained by writing the equations of motion in dimensionless form are
and .
SOLUTION
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