Consider there is only one cylinder, not a concentric one. The cylinder is infinitely long and filled with a Newtonian fluid. The cylinder is rotated at an angular velocity of omega at t>0. Derive the time dependent veloecity profile
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Consider there is only one cylinder, not a concentric one. The cylinder is infinitely long and filled with a Newtonian fluid. The cylinder is rotated at an angular velocity of omega at t>0. Derive the time dependent veloecity profile
Thankfully, you were able to reconnect your air tube before you lost consciousness. After such a stressful situation, you decided to take a vacation. On your vacation, you are sitting on a beach on Earth drinking a cocktail (a non-alcoholic one, of course). It's one of those fancy drinks with a straw, as shown below on the left. As an engineer who is fascinated by fluid flow, you start wondering about the velocity profiles within the fluid that you create...
Navier-Stokes Equation: An incompressible Newtonian liquid is confined between two concentric cylinders of infinite length—a solid inner cylinder of radius RA and a hollow outer cylinder of radius RB. The inner cylinder rotates at angular velocity ω and the outer cylinder is stationary. The flow is steady, laminar, and two-dimensional in the r-θ plane. The flow is rotationally symmetric, meaning that nothing is a function of the coordinate θ. The flow is also circular so that ur=0 everywhere. Found Uθ=...
An incompressible Newtonian fluid is contained between two long concentric cylinders of radii AR (< 1) and R, as shown in the figure. The inner cylinder rotates with an angular velocity Ω (a) Compute the velocity distribution between the cylinders. End effects caused by (b) Compute the torque required to hold the outer cylinder stationary. (8 Pts) An incompressible Newtonian fluid is contained between two long concentric cylinders of radii AR (
Consider two concentric, infinitely long cylinders. The cylinders are oriented such that the center-line is along the z-axis, and the radii exist in the r-direction. The inner cylinder has a radius of ra and the outer cylinder has a radius Tb. The inner cylinder rotates with an angular velocity of w whereas the outer cylinder is stationary. There is no pressure gradient applied nor gravity. The fluid contained between the cylinders is assumed to be Netwonian, incompressible, isotropic and isothermal....
Consider two concentric, infinitely long cylinders. The cylinders are oriented such that the center-line is along the z-axis, and the radii exist in the r-direction. The inner cylinder has a radius of ra and the outer cylinder has a radius rb. The inner cylinder moves in the positive z-direction with a velocity W while the outer cylinder is held stationary. The fluid contained between the cylinders is assumed to be Netwonian, incompressible, isotropic and isothermal. The flow of the fluid...
A viscometer is an instrument for measuring the viscosity of a fluid. In a simple form, it consists of two concentric cylinders, with the outer cylinder fixed and the inner cylinder free to rotate. The space between the two cylinders is filled with the fluid in question, and the torque required to rotate the inner cylinder at a constant speed is measured. One such device consists of two 21.0-cm long cylinders, one 15 cm in diameter and the other 15.4...
Fluid is Non-Newtonian. (3) Consider the steady laminar flow between the coaxial cylinders shown below. The inner cylinder rotates with angular velocity 2 and the outer cylinder is stationary. The no-slip condition applies at the inner and outer cylinder surfaces and we are considering the cylinders to be very long in the 2-direction hence we may ignore edge effects near the top and bottom surfaces. - R2 Assume that gravity is negligible, v, is zero and that are zero for...
The device shown in Figure OA3 is called a cone-plate viscometer. The angle of the cone is very small, so that sin 0 0, and the gap is filled with the test liquid. The torque M to rotate the cone at the angular velocity Q is measured. Assuming a linear fluid velocity profile along the thickness of the fluid film and non-slip boundary condition at the surfaces of the solid bodies, derive an expression for fluid dynamic viscosity u as...
Page 5 Nane: Johnson, Perri NN: 35 1000 omawork 10 10.5 Aoni cous fuid is contained betwen two infinitely vertical, concentric cylinders. The outer cylinder has a radius fixedd rotates with an angular velocity o. The inner cylinder is and has a radius r. The Navier-Stokes equations can be used As utain an exact solution for the velocity distribution in the gap. that the flow in the gap is axisymmetric (neither velocity Fluid nor pressure are functions of angular position...