phy-4600/lecture_notes/2-29/overview
2016-03-25 20:08:04 -04:00

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Problems with known polarization
(pic) Uniformly polarized sphere
Gauss' Law in Dielectric
ε₀∇⋅𝐄 = ρ = ρfree + ρbound
= ρfree - ∇⋅𝐏
ε₀∇⋅𝐄 + ∇⋅𝐏 = ρfree
∇⋅(ε₀𝐄 + 𝐏) = ρfree/ε₀
𝐃 ≡ ε₀𝐄 + 𝐏
Bar Electret
- Analogous to Magnetic bar
Two limits and an intermediate case.
∇×𝐃 = ∇×(ε₀𝐄 + 𝐏) = ∇×𝐏
𝐄 for bar electret, properties:
(𝐄₂ - 𝐄₁)⋅𝐧̂₁→₂ = σ/ε₀ with σ = σᵦ + σfree
Curl eq shows 𝐄"₂ - 𝐄"₁ = 0 (tangential components).
(𝐃₂ - 𝐃₁)⋅𝐧̂₁→₂ = σfree
(𝐃"₂ - 𝐃"₁) = 𝐏"₂ - 𝐏"₁
𝐏 = ε₀χₑ𝐄
• χₑ is the susceptibility of a linear dielectric material.
𝐃 = ε₀𝐄 + 𝐏 = ε₀𝐄 + ε₀χₑ𝐄 = ε₀(1+χₑ) 𝐄
• ε₀(1+χₑ) ≡ permittivity
• 1+χₑ = dielectric constant
Metal Sphere
(pic) What is V(0)?
(pic) ε becomes relevant in electric field
𝐄 = ⎧ 𝐃/ε = Q𝐫̂/(4πεr²), R<r<b
𝐃/ε = Q𝐫̂/(4πε₀r²), b<r
R b ∞
V(∞) - V(0) = -∫ 𝐄⋅d𝐥 - ∫ 𝐄⋅d𝐥 - ∫ 𝐄⋅d𝐥
0 R b
= 0 - ...