Step 1: Understand the concept
Brewster's law says that at the polarising angle \(\theta\), \(\tan\theta = \mu\), where \(\mu\) is the refractive index of glass relative to air.
Step 2: Link \(\mu\) with wavelength
The frequency does not change on entering glass, so \(\mu = \dfrac{c}{v} = \dfrac{\lambda_a}{\lambda_g}\).
Step 3: Combine
\[ \tan\theta = \frac{\lambda_a}{\lambda_g} \Rightarrow \lambda_g = \frac{\lambda_a}{\tan\theta} = \lambda_a\cot\theta \]
Step 4: Result
Option (B). Option (A) has \(\lambda_a\) and \(\lambda_g\) interchanged, and the \(\tan^2\theta\) options have a wrong power of the tangent.
Final Answer:
lambda_g = lambda_a cot theta. This is option (B).
\[ \boxed{\text{(B) }\lambda_g=\lambda_a\cot\theta} \]