16. The magnetic flux through three different coils is changing as shown in Figure P21.160. For each situation, draw a corresponding graph showing qualitatively how the induced emf changes with time. Figure P21.16 (a) Φ (b) Φ (c) Φ KAT h t

16. The magnetic flux through three different coils is changing as shown in Figure P21.160. For each situation, draw a corresponding graph showing qualitatively how the induced emf changes with time. Figure P21.16 (a) Φ (b) Φ (c) Φ KAT h t

College Physics

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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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Concept explainers

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

16. The magnetic flux through three different coils is changing as shown in Figure P21.160.
For each situation, draw a corresponding graph showing qualitatively how the induced
emf changes with time.
Figure P21.16
(a) Φ
(b) Φ
KAR

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17. The magnetic flux through three different coils is changing as shown in Figure P21.17. For each situation, draw a corresponding graph showing quantitatively how the induced emf changes with time. FIGURE P21.17 $(T•m²) 0.4 0.2 0 0 2 4 (T • mỏ) 0.4 0 01234 p(T•mỏ) +0.2 A 1 2 3 t(s) -0.2 -t (s)