Find the total magnetic force acting on the loop abc. 60 a O a. F= 21LB cos(60); down O b. F= 21LB cos(60); out of the page O c. F=ILB cos(60); up O d. F= ILB sin(60); to the right O e. F = ILB sin(60); to the left O f. F= 0 g. F = ILB; to the right O h. F= ILB sin(60); into the page

Find the total magnetic force acting on the loop abc. 60 a O a. F= 21LB cos(60); down O b. F= 21LB cos(60); out of the page O c. F=ILB cos(60); up O d. F= ILB sin(60); to the right O e. F = ILB sin(60); to the left O f. F= 0 g. F = ILB; to the right O h. F= ILB sin(60); into the page

College Physics

11th Edition

ISBN:9781305952300

Author:Raymond A. Serway, Chris Vuille

Publisher:Raymond A. Serway, Chris Vuille

Chapter1: Units, Trigonometry. And Vectors

Section: Chapter Questions

Problem 1CQ: Estimate the order of magnitude of the length, in meters, of each of the following; (a) a mouse, (b)...

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Magnetic Field Of Coaxial Cable

The word coaxial means same axis. So for a long straight cable to be coaxial, it must have concentric cylindrical shaped conductor around it. Coaxial cable (popularly called ‘coax’) has various applications ranging from current conductors to radiofrequency signal transmitters. This cable has lower emission losses and provides protection from electromagnetic interference which allows signals with less power to transmit over longer distances.For example, currents produced in the pickup of a stereo turntable generally travel to the amplifier through a coaxial cable.The self-inductance of a coaxial cable is another important characteristic, because it influences the propagation of electrical signals in the cable.

Question

Find the total magnetic force acting on the loop abc.
60
a
O a. F= 21LB cos(60); down
O b. F= 21LB cos(60); out of the page
O c. F=ILB cos(60); up
O d. F= ILB sin(60); to the right
O e.
F = ILB sin(60); to the left
O f. F= 0
g.
F = ILB; to the right
O h. F= ILB sin(60); into the page

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