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1 運動する系から見た電磁気学 - 東京大学

A = −µ 0i (6) divA + µε 0 ∂φ ∂t = 0 (7) に帰着される。また電荷の保存則 divi+ ∂ρ ∂t = 0 (8) を満たす必要がある。これら方程式がガリレイ変換に対してどうなるかを考えてみよう。

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