Elements Of Electromagnetics
7th Edition
ISBN: 9780190698614
Author: Sadiku, Matthew N. O.
Publisher: Oxford University Press
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- Find the resultant force in the y-direction Fr,y for a volumetric flow rate in the y direction of 100 L/hr, a pressure of 150 kPa, and a diameter of 3 cm. Use the equation Fr, y = -m1y1 - P1A1arrow_forwardsimple answer no need to explainarrow_forward1. A water jetpack suspends a 7Okg man in air without motion along the vertical and the horizontal as the man tilts the platform. The jetpack has two outlets, each has a diameter of 5cm, and an inlet with a diameter of 6cm. Calculate the volumetric flowrate, in and out of the water jetpack, and the angle 00 such that there is no motion along any direction. Neglect the weight of the jetpack. The inlet is perpendicular to the outlet. inlet W W Qi 2Q. ВАCK SIDEarrow_forward
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- A 30º reducing elbow is shown. The fluid is water. Evaluate the components of force that must be provided by the adjacent pipes to keep the elbow from moving. Assume steady, incompressible, uniform flow. ρwater= 999kg/m3, Q= 0.11 m3/s.1 atm = 101 kPa;arrow_forwardConsider an airplane flying with a velocity of 60ft/s at a standard sea level conditions. At a point on the wing, the airflow velocity is 70ft/s. Calculate the pressure at this point. Assume the incompressible flow.arrow_forwardProblem Consider a cylindrical pipe of length L and diameter D = 2R. The angle that the axis of the pipe forms with the vertical direction is a. Assume that when the fluid enters the pipe its velocity is uniform (i.e., it has the same value over the entire cross-section of the pipe) and equal to U in the axial direction. In the radial and angular directions, the velocity is zero. So, it is: 2 =0: v(r, 0, 2) = Ue, (1.1) Here v is the fluid velocity and e, is a vector of unit magnitude parallel to the coordinate axis z; furthermore, we have assumed that the pipe inlet is located at z = 0. Near the entrance of the pipe, the velocity profile varies in the axial direction. But after a certain entrance length, the profile becomes fully developed, no longer changing with z. The evolution of the velocity profile is sketched in Fig. 1, where, for clarity, the pipe inclination is not shown. The entrance length is denoted by L.. For z > L., the fluid velocity is no longer a function of the axial…arrow_forward
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