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At the uncharged interface between two linear dielectrics with permitivities \(\epsilon_{1}\) and \(\epsilon_{2}\), electric fields \(\overline{E_{1}}\) and \(\overline{E_{2}}\) make angles \(\theta_{1}\) and \(\theta_{2}\) with the normal. The ratio \(\epsilon_{1} / \epsilon_{2}\) is equal to :

  • A.\(\tan\theta_{1}/\tan\theta_{2}\)
  • B.\(\sin\theta_{1}/\sin\theta_{2}\)
  • C.\(\cos\theta_{1}/\cos\theta_{2}\)
  • D.\(\cot\theta_{1}/\cot\theta_{2}\)

Answer: A

The ratio is \(\epsilon_{1}/\epsilon_{2} = \tan\theta_{1}/\tan\theta_{2}\).

At an uncharged interface the tangential component of E and the normal component of D are continuous:

\[ \begin{aligned} E_{1}\sin\theta_{1} &= E_{2}\sin\theta_{2} \\ \epsilon_{1}E_{1}\cos\theta_{1} &= \epsilon_{2}E_{2}\cos\theta_{2} \end{aligned} \]

Dividing the first equation by the second gives \(\tan\theta_{1}/\epsilon_{1} = \tan\theta_{2}/\epsilon_{2}\), the law of refraction of field lines.

The sine ratio is Snell's law for light, which involves refractive indices rather than permittivities. The cosine and cotangent ratios do not follow from the boundary conditions; the cotangent ratio is in fact the inverse of the correct answer.

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