જો \(\lambda_0\) અને \(\lambda\) અનુક્રમે દેહલીજ તરંગલંબાઈ આપાત પ્રકાશની તરંગલંબાઈ હોય તો ધાતુની સપાટી પરથી મુક્ત થતા ફોટોઇલેક્ટ્રોનનો વેગ જણાવો.

A \(\sqrt {\frac{{2h}}{m}\left( {{\lambda _0} - \lambda } \right)} \)
B \(\sqrt {\frac{{2hc}}{m}\left( {{\lambda _0} - \lambda } \right)} \)
C \(\sqrt {\frac{{2hc}}{m}\left( {\frac{{{\lambda _0} - \lambda }}{{\lambda {\lambda _0}}}} \right)} \)
D \(\sqrt {\frac{{2h}}{m}\left( {\frac{1}{{{\lambda _0}}} - \frac{1}{\lambda }} \right)} \)

Verified Solution

Answer & Solution

Correct Answer

(C) \(\sqrt {\frac{{2hc}}{m}\left( {\frac{{{\lambda _0} - \lambda }}{{\lambda {\lambda _0}}}} \right)} \)

Step-by-step Solution

Detailed explanation

The kinetic enegry of the ejected electron is given by the equation \(hv = h{v_0} + \frac{1}{2}m{v^2}\,\,\,\because \,v = \frac{c}{\lambda }\) or \(\frac{{hc}}{\lambda } = \frac{{hc}}{{{\lambda _0}}} + \frac{1}{2}m{v^2}\)…

Apply the relevant identity from the chapter and substitute the values established in the previous step, keeping the original constraint in view.

Use the simplified expression to isolate the unknown, then plug the result back into the question setup to confirm the working is internally consistent.

Cross-check against a boundary or limiting case. Both the dimensional balance and the qualitative behaviour at the extreme should agree with the candidate answer.

Combine the steps above to identify the correct option. The remaining choices each fail at least one of the consistency, dimensional, or boundary checks.

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