Page 58 - Electric Machinery Fundamentals
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34   ELECTRJC MACHINERY FUNDAMENTALS

             Therefore,
                                   F = 0.125 N,  directed to the right

                  The induction of a force in a wire by a cun-ent in the presence of a magnetic
             field is  the  basis of motor action.  Almost every  type of motor depends  on  this
             basic principle for the forces and torques which make it move.
             1.7  INDUCED VOLTAGE ON A CONDUCTOR
             MOVING IN A MAGNETIC FIELD
             There is a third major way in which a magnetic field interacts with its surround-
             ings. If a wire with the proper orientation moves through a magnetic field, a volt-
             age is induced in it. This idea is shown in Figure 1-17. The voltage induced in the
             wire is given by
                                       eiod  =  (v X B) • 1              (1-45)

             where
                   v  =  velocity of the wire
                  B  =  magnetic flux density vector
                   I =  length of conductor in the magnetic field
             Vector I points along the direction of the wire toward the end making the smallest
             angle with respect to the vector v  X B. The voltage in the wire will be built up so
             that the positive end is  in the direction of the vector v  X B. The following exam-
             ples illustrate this concept.
                  Example  1- 8.  Figure 1- 17 shows a conductor moving with a velocity of 5.0 m/s
             to the right in the presence of a magnetic field. The flux density is 0.5 T into the page, and
             the wire is 1.0 m in  length, oriented as shown. What are the magnitude and polarity  of the
             resulting induced voltage?
                  Solution
             The direction of the quantity v X B in this example is up. Therefore, the voltage on the con-
             ductor will be built up positive at the top with respect to the bottom of the wire. The direc-
             tion of vector I is up, so that it makes the smallest angle with respect to the vector v X B.
                  Since v is  perpendicular to B and since v  X B is parallel to I, the magnitude of the
             induced voltage reduces to
                                    eind  = (v X  B) -I                (1-4S)
                                       =  (vB sin 900) I cos 0°
                                       =  vBI
                                       ~ (S.O mls)(O.S T)(1.0 m)
                                       ~ 2.SV
                  Thus the induced voltage is 2.5 V, positive at the top of the wire.
                                                                                (
                  Example 1- 9.  Figure 1-18 shows a conductor moving with a velocity of 10 m/s
             to the right in a magnetic field. The flux density is 0.5 T,  out of the page, and the wire is
             1.0 m in length, oriented as  shown. What are the magnitude and polffi"ity of the resulting
             induced voltage?
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