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CHAPTER 7   The Steady Magnetic Field         181
















                                       Figure 7.1 The law of Biot-Savart
                                       expresses the magnetic field intensity dH 2
                                       produced by a differential current element
                                       I 1 dL 1 . The direction of dH 2 is into the
                                       page.

                     case of a cylindrical conductor of circular cross section as the radius approaches zero.
                     We assume a current I flowing in a differential vector length of the filament dL. The
                                    1
                     law of Biot-Savart then states that at any point P the magnitude of the magnetic
                     field intensity produced by the differential element is proportional to the product of
                     the current, the magnitude of the differential length, and the sine of the angle lying
                     between the filament and a line connecting the filament to the point P at which
                     the field is desired; also, the magnitude of the magnetic field intensity is inversely
                     proportional to the square of the distance from the differential element to the point P.
                     The direction of the magnetic field intensity is normal to the plane containing the
                     differential filament and the line drawn from the filament to the point P.Of the two
                     possible normals, that one to be chosen is the one which is in the direction of progress
                     of a right-handed screw turned from dL through the smaller angle to the line from the
                     filament to P. Using rationalized mks units, the constant of proportionality is 1/4π.
                         The Biot-Savart law, just described in some 150 words, may be written concisely
                     using vector notation as
                                                           IdL × R
                                                IdL × a R
                                          dH =           =                            (1)
                                                  4πR 2     4πR 3
                     The units of the magnetic field intensity H are evidently amperes per meter (A/m).
                     The geometry is illustrated in Figure 7.1. Subscripts may be used to indicate the point
                     to which each of the quantities in (1) refers. If we locate the current element at point 1
                     and describe the point P at which the field is to be determined as point 2, then

                                                    I 1 dL 1 × a R12
                                              dH 2 =                                  (2)
                                                           2
                                                       4πR 12


                     1  Biot and Savart were colleagues of Amp`ere, and all three were professors of physics at the Coll`ege de
                     France at one time or another. The Biot-Savart law was proposed in 1820.
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