Page 343 - Schaum's Outline of Theory and Problems of Applied Physics
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328                                    MAGNETISM                                 [CHAP. 27



                  Bar magnets with poles facing each other are equivalent to parallel current loops whose currents are in opposite
              directions [Fig. 27-12(a)]. Such loops repel. Bar magnets with opposite poles facing each other are equivalent to
              parallel current loops whose current loops are in the same direction [Fig. 27-12(b)]. Such loops attract.



                                 S  N      N  S


                                   Like poles repel      Parallel loops with opposite currents repel
                                                      (a)



                                  S  N     S  N

                                  Unlike poles attract   Parallel loops with similar currents attract
                                                      (b)
                                                    Fig. 27-12



        SOLVED PROBLEM 27.16
              How does a permanent magnet attract an unmagnetized iron object?
                  The presence of the magnet induces the atomic magnets in the object to line up with its field (Fig. 27-13), and
              the attraction of opposite poles then produces a net force on the object.




                             S         N




                             S         N


                                                    Fig. 27-13



        SOLVED PROBLEM 27.17
              An unmagnetized iron rod is placed inside a solenoid. The current in the solenoid is then increased
              from zero to a maximum in one direction, decreased back to zero, increased to a maximum in the other
              direction, brought back to zero, and so on. Plot B versus H for the iron rod, and discuss the shape of the
              resulting curve.
                  The required curve is shown in Fig. 27-14. At a, both H and B are 0. As H increases, B increases slowly at
              first, then rapidly, and finally levels off at a maximum value at b. The rod is now saturated, and a further increase
              in H will not change B. Saturation occurs when all the magnetic domains in the rod are aligned with H. The curve
              from a to b is called the magnetization curve of the material.
                  When H is brought back to 0 from H b , B lags behind so that B = B c at point c when H = 0. This is an example
              of hysteresis. The value of B c is called the retentivity of the material. To demagnetize the rod completely, H must
              be reversed in direction and increased to H d , the coercive force. The greater the retentivity, the stronger the residual
              magnetization of the rod; the greater the coercive force, the better able the rod will be to keep its magnetization
              despite the presence of strong magnetic fields. Thus a good material for a permanent magnet should have both a high
              retentivity and a high coercive force.
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