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Photoelectric emission is observed from ...

Photoelectric emission is observed from a surface for frequencies `v_(1) "and" v_(2)` of the incident radiation `(v_(1) gt v_(2))` . If maximum kinetic energies of the photo electrons in the two cases are in the ratio `1:K` , then the threshold frequency is given by:

A

`(v_(2)-v_(1))/(K-1)`

B

`(Kv_(1)-v_(2))/(K-1)`

C

`(Kv_(2)-v_(1))/(K-1)`

D

`(v_(2)-v_(1))/K`

Text Solution

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The correct Answer is:
To solve the problem, we will use the principles of the photoelectric effect. The key points to remember are: 1. The energy of the incident photon is given by \( E = h \nu \), where \( h \) is Planck's constant and \( \nu \) is the frequency of the incident radiation. 2. The maximum kinetic energy (KE) of the emitted photoelectrons can be expressed as: \[ KE = h \nu - \phi \] where \( \phi \) is the work function of the material, which is related to the threshold frequency \( \nu_0 \) by \( \phi = h \nu_0 \). ### Step-by-step Solution: 1. **Write the equations for the maximum kinetic energies:** For the two frequencies \( \nu_1 \) and \( \nu_2 \): \[ KE_1 = h \nu_1 - h \nu_0 \quad (1) \] \[ KE_2 = h \nu_2 - h \nu_0 \quad (2) \] 2. **Express the kinetic energies in terms of the threshold frequency:** From equations (1) and (2), we can express the kinetic energies as: \[ KE_1 = h (\nu_1 - \nu_0) \] \[ KE_2 = h (\nu_2 - \nu_0) \] 3. **Set up the ratio of the kinetic energies:** According to the problem, the maximum kinetic energies are in the ratio \( 1:K \): \[ \frac{KE_1}{KE_2} = \frac{1}{K} \] Substituting the expressions for \( KE_1 \) and \( KE_2 \): \[ \frac{h (\nu_1 - \nu_0)}{h (\nu_2 - \nu_0)} = \frac{1}{K} \] 4. **Simplify the equation:** The \( h \) cancels out: \[ \frac{\nu_1 - \nu_0}{\nu_2 - \nu_0} = \frac{1}{K} \] Cross-multiplying gives: \[ K (\nu_1 - \nu_0) = \nu_2 - \nu_0 \] 5. **Rearranging for the threshold frequency \( \nu_0 \):** Rearranging the equation: \[ K \nu_1 - K \nu_0 = \nu_2 - \nu_0 \] \[ K \nu_1 - \nu_2 = K \nu_0 - \nu_0 \] \[ K \nu_1 - \nu_2 = (K - 1) \nu_0 \] Finally, solving for \( \nu_0 \): \[ \nu_0 = \frac{K \nu_1 - \nu_2}{K - 1} \] ### Final Answer: The threshold frequency \( \nu_0 \) is given by: \[ \nu_0 = \frac{K \nu_1 - \nu_2}{K - 1} \]

To solve the problem, we will use the principles of the photoelectric effect. The key points to remember are: 1. The energy of the incident photon is given by \( E = h \nu \), where \( h \) is Planck's constant and \( \nu \) is the frequency of the incident radiation. 2. The maximum kinetic energy (KE) of the emitted photoelectrons can be expressed as: \[ KE = h \nu - \phi \] where \( \phi \) is the work function of the material, which is related to the threshold frequency \( \nu_0 \) by \( \phi = h \nu_0 \). ...
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