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After defining the derivative maxwell's equations are reduced to a single equation, maxwell's equations aps formulation in three dimensions, the derivative has a special structure allowing the introduction of a cross product: from which it is easily seen that gauss's law is the scalar part, the ampAtildeumlreacirceuroldquomaxwell law is the vector part, faraday's law is the pseudovector part, and gauss's law for magnetism is the pseudoscalar part of the equation Taubman william s