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在幹麻~
※ 引述《Hydrisk (莎莉絲)》之銘言:
: Poyntiny's Theorem
: We = ε/2 (E‧E)
: Wm = 1/2μ(B‧B)
: Uem = 1/2(ε(E‧E) + 1/μ(B‧B))
: Uem is called energy density
: Accroding to the Lorentz force law
: F‧dl = q(E + V ×B)‧Vdt
: magnetic forces do no work
: F‧dl = qE‧Vdt
: q = ρdτ
: F‧dl = E‧ρVdτdt
: dW/dt = ∫(E‧J)dτ
: Accroding to the Ampere's law with Maxwell's equation correction
: ▽ ×B = μJ+εμ(dE/dt)
: J = 1/μ(▽ ×B) - ε(dE/dt)
: => dW/dt = ∫(1/μE‧(▽ ×B) - εE‧(dE/dt))dτ
: E‧(▽ ×B) = B‧(▽ ×E) - ▽‧(E ×B)
: Accroding to the Faraday's law
: ▽ ×E = -(dB/dt)
: => E‧(▽ ×B) = -B‧(dB/dt) - ▽‧(E ×B)
: dW/dt = ∫(-1/μB‧(dB/dt) - εE‧(dE/dt))dτ - 1/μ▽‧(E ×B))dτ
: B‧(dB/dt) = 1/2(d(B‧B)/dt) E‧(dE/dt) = 1/2(d(E‧E)/dt)
: dW/dt = (d/dt)(-1/2)∫(ε(E‧E) + 1/μ(B‧B))dτ - 1/μ∮(E ×B)‧da
: Poynting's vector S = 1/μ(E ×B)
: The first integral on the right is the tatle energy in the electromagnetic
: field.While the sencond integral is the energy flow on boundary surface of
: the volume V.
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