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\/>\n\\mathcal{E} = -\\frac{d\\Phi_B}{dt}<br \/>\n\\]<\/p>\n<p>\u3053\u3053\u3067\u3001<br \/>\n&#8211; \\(\\mathcal{E}\\) \u306f\u8a98\u5c0e\u8d77\u96fb\u529b\uff08\u96fb\u5727\uff09\u3092\u6307\u3057\u307e\u3059\u3002<br \/>\n&#8211; \\(\\Phi_B\\) \u306f\u78c1\u675f\u3092\u793a\u3057\u307e\u3059\u3002<br \/>\n&#8211; \\(\\frac{d\\Phi_B}{dt}\\) \u306f\u6642\u523b \\(t\\) \u306b\u304a\u3051\u308b\u78c1\u675f \\(\\Phi_B\\) 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