Polarization vector
P = χ ϵ 0 E P=\chi \epsilon_0 E P = χ ϵ 0 E
ϵ = 1 + χ → χ = ϵ − 1 = 4 − 1 = 3 \epsilon=1+\chi \to \chi=\epsilon-1=4-1=3 ϵ = 1 + χ → χ = ϵ − 1 = 4 − 1 = 3
P = χ ϵ 0 E = 3 ⋅ 8.85 ⋅ 1 0 − 12 ⋅ 100 = 26.55 ⋅ 1 0 − 10 F ⋅ V m 2 P=\chi \epsilon_0 E=3\cdot 8.85\cdot 10^{-12}\cdot 100=26.55\cdot 10^{-10} \frac{F\cdot V}{m^2} P = χ ϵ 0 E = 3 ⋅ 8.85 ⋅ 1 0 − 12 ⋅ 100 = 26.55 ⋅ 1 0 − 10 m 2 F ⋅ V
Molecular/atomic polarisability
P = N α ϵ 0 E → α = P N ϵ 0 E = 26.55 ⋅ 1 0 − 10 6.02 ⋅ 1 0 23 ⋅ 8.85 ⋅ 1 0 − 12 ⋅ 100 = 0.5 ⋅ 1 0 − 23 m 3 P=N\alpha \epsilon_0 E \to \alpha=\frac{P}{N \epsilon_0 E}=\frac{26.55\cdot 10^{-10}}{6.02\cdot 10^{23}\cdot 8.85\cdot 10^{-12}\cdot 100}=0.5\cdot 10^{-23} m^3 P = N α ϵ 0 E → α = N ϵ 0 E P = 6.02 ⋅ 1 0 23 ⋅ 8.85 ⋅ 1 0 − 12 ⋅ 100 26.55 ⋅ 1 0 − 10 = 0.5 ⋅ 1 0 − 23 m 3
Refractive index
n = ϵ μ = 4 ⋅ 0.99 = 1.99 n=\sqrt{\epsilon\mu}=\sqrt{4\cdot 0.99}=1.99 n = ϵ μ = 4 ⋅ 0.99 = 1.99