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If light of wavelength lambda(1) is allo...

If light of wavelength `lambda_(1)` is allowed to fall on a metal , then kinetic energy of photoelectrons emitted is `E_(1)`. If wavelength of light changes to `lambda_(2)` then kinetic energy of electrons changes to `E_(2)`. Then work function of the metal is

A

`(E_(1)E_(2)(lambda_(1)-lambda_(2)))/(lambda_(1)lambda_(2))`

B

`(E_(1)lambda_(1)-E_(2)lambda_(2))/(lambda_(1)-lambda_(2))`

C

`(E_(1)lambda_(1)-E_(2)lambda_(2))/(lambda_(2)-lambda_(1))`

D

`(lambda_(1)lambda_(2)E_(1)E_(2))/(lambda_(2)-lambda_(1))`

Text Solution

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The correct Answer is:
To find the work function of the metal based on the given wavelengths and kinetic energies of emitted photoelectrons, we will use Einstein's photoelectric equation. Here’s a step-by-step solution: ### Step 1: Write down Einstein's photoelectric equation Einstein's photoelectric equation is given by: \[ E = \frac{hc}{\lambda} = \phi + KE \] where: - \( E \) is the energy of the incident photon, - \( \phi \) is the work function of the metal, - \( KE \) is the kinetic energy of the emitted photoelectron, - \( h \) is Planck's constant, - \( c \) is the speed of light, - \( \lambda \) is the wavelength of the incident light. ### Step 2: Apply the equation for the first wavelength \( \lambda_1 \) For the first case where the wavelength is \( \lambda_1 \) and the kinetic energy is \( E_1 \): \[ \frac{hc}{\lambda_1} = \phi + E_1 \] This can be rearranged to: \[ \phi = \frac{hc}{\lambda_1} - E_1 \quad \text{(Equation 1)} \] ### Step 3: Apply the equation for the second wavelength \( \lambda_2 \) For the second case where the wavelength is \( \lambda_2 \) and the kinetic energy is \( E_2 \): \[ \frac{hc}{\lambda_2} = \phi + E_2 \] This can be rearranged to: \[ \phi = \frac{hc}{\lambda_2} - E_2 \quad \text{(Equation 2)} \] ### Step 4: Set the two expressions for work function equal to each other Since both equations equal \( \phi \), we can set them equal to each other: \[ \frac{hc}{\lambda_1} - E_1 = \frac{hc}{\lambda_2} - E_2 \] ### Step 5: Rearrange the equation to isolate \( hc \) Rearranging gives: \[ \frac{hc}{\lambda_1} - \frac{hc}{\lambda_2} = E_1 - E_2 \] Factoring out \( hc \): \[ hc \left( \frac{1}{\lambda_1} - \frac{1}{\lambda_2} \right) = E_1 - E_2 \] ### Step 6: Solve for \( hc \) Now, we can solve for \( hc \): \[ hc = \frac{(E_1 - E_2)}{\left( \frac{1}{\lambda_1} - \frac{1}{\lambda_2} \right)} \] ### Step 7: Substitute \( hc \) back into one of the equations for \( \phi \) We can substitute \( hc \) back into either Equation 1 or Equation 2. Let’s use Equation 1: \[ \phi = \frac{(E_1 - E_2)}{\left( \frac{1}{\lambda_1} - \frac{1}{\lambda_2} \right) \cdot \frac{1}{\lambda_1}} - E_1 \] ### Step 8: Final expression for work function \( \phi \) After simplifying, we can express the work function \( \phi \) as: \[ \phi = \frac{E_1 \lambda_1 - E_2 \lambda_2}{\lambda_1 - \lambda_2} \] ### Conclusion Thus, the work function of the metal is given by: \[ \phi = \frac{E_1 \lambda_1 - E_2 \lambda_2}{\lambda_1 - \lambda_2} \]
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