Step 1: Understanding the Concept:
Newton's rings are formed due to interference between light waves reflected from the top and bottom surfaces of a thin air film trapped between a plano-convex lens and a flat glass plate. A key aspect is the phase change of \(\pi\) (or path difference of \(\lambda/2\)) that occurs upon reflection from a denser medium.
Step 2: Key Formula or Approach:
1. Light traveling from a rarer medium (air) reflects off the surface of a denser medium (the bottom glass plate). This reflection introduces a phase shift of \(\pi\), which is equivalent to an extra path difference of \(\lambda/2\).
2. The reflection from the top surface (the bottom of the lens) is from a rarer medium (glass) to a denser medium (air), so there is no phase shift here.
3. The geometrical path difference for a wave that travels through the film of thickness 't' and back is \(2t\) (assuming near-normal incidence).
4. The total optical path difference is \( \Delta = 2t + \frac{\lambda}{2} \).
5. For constructive interference (a bright fringe), the total path difference must be an integer multiple of the wavelength: \( \Delta = m\lambda \), where \(m = 1, 2, 3, ...\).
Step 3: Detailed Explanation:
Setting the condition for a bright fringe:
\[ \text{Total path difference} = m\lambda \]
\[ 2t + \frac{\lambda}{2} = m\lambda \]
Solving for \(2t\):
\[ 2t = m\lambda - \frac{\lambda}{2} \]
\[ 2t = \left(m - \frac{1}{2}\right)\lambda \]
\[ 2t = \frac{(2m-1)\lambda}{2} \]
This matches option (C). Option (A) is also mathematically equivalent, but option (C) is a more standard representation.
Step 4: Final Answer:
The condition for a bright ring is \( 2t = \frac{(2m-1)\lambda}{2} \).