Elements Of Electromagnetics
7th Edition
ISBN: 9780190698614
Author: Sadiku, Matthew N. O.
Publisher: Oxford University Press
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A solid cone of angle 2Ɵ, base r 0 , and density ρ c is rotating with initial
angular velocity ω 0 inside a conical seat,
as shown below. The clearance h is filled with oil
of viscosity μ. Neglecting air drag, derive an analytical expression for the
cone’s angular velocity ω(t) if there is no
applied torque.
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- A solid cone of angle 2θ , base r 0 , and density ρ c is rotatingwith initial angular velocity ω 0 inside a conical seat, asshown in Fig. . The clearance h is fi lled with oil ofviscosity μ . Neglecting air drag, derive an analyticalexpression for the cone’s angular velocity ω ( t ) if there isno applied torque.arrow_forwardIn studying sand transport by ocean waves, A. Shields in1936 postulated that the threshold wave-induced bottomshear stress τ required to move particles depends on gravityg , particle size d and density ρ p , and water density ρ andviscosity μ . Find suitable dimensionless groups of thisthe problem, which resulted in 1936 in the celebrated Shieldssand transport diagram.arrow_forwardBy using the expression for the shear stress derived in class (and in BSL), show that the shear force on asphere spinning at a constant angular velocity in a Stokes’ flow, is zero.This means that a neutrally buoyant sphere (weight equal buoyancy force) that is made to spin in aStokes’ flow, will neither rise nor fall, nor translate in any preferential direction in the (x-y) plane. expressions for velocity are: v_r (r,θ)= U_∞ [1-3R/2r+R^3/(2r^3 )] cosθ v_θ (r,θ)= -U_∞ [1-3R/4r-R^3/(4r^3 )] sinθ Where v_r and v_θ are the radial and angle velocity, U_∞ is the velocity of fluid coming to sphere which very faar away from the sphere. And R is the radius of sphere.arrow_forward
- 3.14. Find the vorticity in polar coordinates for the following velocity com- ponents (a) v=rsin 0, ve = 2r cos 0 (b) v = cos 0, 11=0arrow_forwardA cube of side (a) and mass (M) is initially sitting fully submerged at the bottom of a container filled with a liquid of kinematic viscosity v and density p. The container has a square cross-section of side (a+a/5) and the cube is sitting right at the middle of the container base. (a) A force (F) starts pulling the cube up at a constant velocity (U). Develop an expression for the force in terms of (U, M. a. g, p and v). You may assume that the velocity in the gap between the cube's sides and the container walls is linear. The expression for (F) is to be valid as long as the cube remains submerged. (b) After the cube reaches the water surface, it continues to be pulled up by the same force. Develop a differential equation for the variation with time of the fraction of the cube that is submerged in water.arrow_forward
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