Vector potential, electromagnetic induction and ‘physical meaning’
Vector potential, electromagnetic induction and ‘physical meaning’
复制标题
矢量势、电磁感应和“物理意义”
DOI:
10.1088/0143-0807/31/4/017
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发表时间:
2010
期刊:
影响因子:
--
通讯作者:
G. Giuliani
中科院分区:
文献类型:
--
作者:
G. Giuliani
A forgotten experiment by André Blondel (1914) proves, as held on the basis of theoretical arguments in a previous paper, that the time variation of the magnetic flux is not the cause of the induced emf; the physical agent is instead the vector potential through the term (when the induced circuit is at rest). The ‘good electromagnetic potentials’ are determined by the Lorenz condition and retarded formulae. Other pairs of potentials derived through appropriate gauge functions are only mathematical devices for calculating the fields; they are not physically related to the sources. The physical meaning of a theoretical term relies, primarily, on theoretical grounds; a theoretical term has a physical meaning if it cannot be withdrawn without reducing the predictive power of a theory or, in a weaker sense, if it cannot be withdrawn without reducing the descriptive proficiency of a theory.