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See Ref. 25, p. 335, problem 7.51
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See Ref. 25, p. 335, problem 7.51. This inclusion of the displacement current density was not actually necessary, for only the real current density is needed in the Biot-Savart law for quasistatic circuits (see David J. Griffiths and Mark A. Heald, "Time-dependent generalizations of the Biot-Savart and Coulomb laws," Am. J. Phys. 59, 111-117 (1991); A. P. French and Jack R. Tessman, "Displacement currents and magnetic fields," ibid. 31, 201-204 (1963); Oleg D. Jefimenko, "Comment on 'On the equivalence of the laws of Biot-Savart and Ampere,' by T. A. Weber and D. J. Macomb [Am. J. Phys. 57, 57-59 (1989)]," ibid. 58, 505 (1990); Edward M. Purcell, Electricity and Magnetism, Berkeley Physics Course, Vol. 2 (McGraw-Hill, New York, 1962), 1st ed., pp. 261-262. Removing the displacement current from Eq. (4) resulted in only small changes to the calculated magnetic fields.
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Displacement currents and magnetic fields
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See Ref. 25, p. 335, problem 7.51. This inclusion of the displacement current density was not actually necessary, for only the real current density is needed in the Biot-Savart law for quasistatic circuits (see David J. Griffiths and Mark A. Heald, "Time-dependent generalizations of the Biot-Savart and Coulomb laws," Am. J. Phys. 59, 111-117 (1991); A. P. French and Jack R. Tessman, "Displacement currents and magnetic fields," ibid. 31, 201-204 (1963); Oleg D. Jefimenko, "Comment on 'On the equivalence of the laws of Biot-Savart and Ampere,' by T. A. Weber and D. J. Macomb [Am. J. Phys. 57, 57-59 (1989)]," ibid. 58, 505 (1990); Edward M. Purcell, Electricity and Magnetism, Berkeley Physics Course, Vol. 2 (McGraw-Hill, New York, 1962), 1st ed., pp. 261-262. Removing the displacement current from Eq. (4) resulted in only small changes to the calculated magnetic fields.
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Comment on 'on the equivalence of the laws of Biot-Savart and Ampere
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by T. A. Weber and D. J. Macomb
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See Ref. 25, p. 335, problem 7.51. This inclusion of the displacement current density was not actually necessary, for only the real current density is needed in the Biot-Savart law for quasistatic circuits (see David J. Griffiths and Mark A. Heald, "Time-dependent generalizations of the Biot-Savart and Coulomb laws," Am. J. Phys. 59, 111-117 (1991); A. P. French and Jack R. Tessman, "Displacement currents and magnetic fields," ibid. 31, 201-204 (1963); Oleg D. Jefimenko, "Comment on 'On the equivalence of the laws of Biot-Savart and Ampere,' by T. A. Weber and D. J. Macomb [Am. J. Phys. 57, 57-59 (1989)]," ibid. 58, 505 (1990); Edward M. Purcell, Electricity and Magnetism, Berkeley Physics Course, Vol. 2 (McGraw-Hill, New York, 1962), 1st ed., pp. 261-262. Removing the displacement current from Eq. (4) resulted in only small changes to the calculated magnetic fields.
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Jefimenko, O.D.1
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35
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0037787574
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See Ref. 25, p. 335, problem 7.51. This inclusion of the displacement current density was not actually necessary, for only the real current density is needed in the Biot-Savart law for quasistatic circuits (see David J. Griffiths and Mark A. Heald, "Time-dependent generalizations of the Biot-Savart and Coulomb laws," Am. J. Phys. 59, 111-117 (1991); A. P. French and Jack R. Tessman, "Displacement currents and magnetic fields," ibid. 31, 201-204 (1963); Oleg D. Jefimenko, "Comment on 'On the equivalence of the laws of Biot-Savart and Ampere,' by T. A. Weber and D. J. Macomb [Am. J. Phys. 57, 57-59 (1989)]," ibid. 58, 505 (1990); Edward M. Purcell, Electricity and Magnetism, Berkeley Physics Course, Vol. 2 (McGraw-Hill, New York, 1962), 1st ed., pp. 261-262. Removing the displacement current from Eq. (4) resulted in only small changes to the calculated magnetic fields.
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Am. J. Phys.
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36
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33744601613
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Berkeley Physics Course, McGraw-Hill, New York, 1st ed.
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See Ref. 25, p. 335, problem 7.51. This inclusion of the displacement current density was not actually necessary, for only the real current density is needed in the Biot-Savart law for quasistatic circuits (see David J. Griffiths and Mark A. Heald, "Time-dependent generalizations of the Biot-Savart and Coulomb laws," Am. J. Phys. 59, 111-117 (1991); A. P. French and Jack R. Tessman, "Displacement currents and magnetic fields," ibid. 31, 201-204 (1963); Oleg D. Jefimenko, "Comment on 'On the equivalence of the laws of Biot-Savart and Ampere,' by T. A. Weber and D. J. Macomb [Am. J. Phys. 57, 57-59 (1989)]," ibid. 58, 505 (1990); Edward M. Purcell, Electricity and Magnetism, Berkeley Physics Course, Vol. 2 (McGraw-Hill, New York, 1962), 1st ed., pp. 261-262. Removing the displacement current from Eq. (4) resulted in only small changes to the calculated magnetic fields.
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Electricity and Magnetism
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Purcell, E.M.1
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