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When a metal surface is illuminated by l...

When a metal surface is illuminated by light wavelengths `400 nm` and `250 nm` , the maximum velocities of the photoelectrons ejected are `upsilon` and `2 v` respectively . The work function of the metal is
`( h = "Planck's constant" , c = "velocity of light in air" )`

A

` 2 hc xx 10^(6) J`

B

` 1.5 hc xx 10^(6) J`

C

` hc xx 10^(6) J`

D

` 0.5 hc xx 10^(6) J`

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The correct Answer is:
To find the work function of the metal when illuminated by light of wavelengths 400 nm and 250 nm, we can use the photoelectric effect equation derived from Einstein's photoelectric equation: 1. **Understanding the Problem**: - We have two wavelengths: \( \lambda_1 = 400 \, \text{nm} \) and \( \lambda_2 = 250 \, \text{nm} \). - The maximum velocities of the photoelectrons are \( v_1 = v \) for \( \lambda_1 \) and \( v_2 = 2v \) for \( \lambda_2 \). 2. **Using the Photoelectric Equation**: The kinetic energy of the emitted photoelectrons can be expressed as: \[ K_{\text{max}} = \frac{1}{2} mv^2 = E_{\text{incident}} - \phi \] where \( E_{\text{incident}} = \frac{hc}{\lambda} \) and \( \phi \) is the work function. 3. **For Wavelength \( \lambda_1 = 400 \, \text{nm} \)**: \[ K_{\text{max},1} = \frac{1}{2} mv^2 = \frac{hc}{400 \times 10^{-9}} - \phi \] Let's denote this equation as (1). 4. **For Wavelength \( \lambda_2 = 250 \, \text{nm} \)**: \[ K_{\text{max},2} = \frac{1}{2} m(2v)^2 = \frac{1}{2} m(4v^2) = 2mv^2 = \frac{hc}{250 \times 10^{-9}} - \phi \] Let's denote this equation as (2). 5. **Equating the Kinetic Energies**: From equation (1): \[ \frac{1}{2} mv^2 = \frac{hc}{400 \times 10^{-9}} - \phi \] From equation (2): \[ 2mv^2 = \frac{hc}{250 \times 10^{-9}} - \phi \] 6. **Expressing \( mv^2 \) from Equation (1)**: Multiply both sides of equation (1) by 2: \[ mv^2 = \frac{hc}{200 \times 10^{-9}} - 2\phi \] 7. **Substituting into Equation (2)**: Substitute \( mv^2 \) from above into equation (2): \[ 2\left(\frac{hc}{200 \times 10^{-9}} - 2\phi\right) = \frac{hc}{250 \times 10^{-9}} - \phi \] 8. **Simplifying the Equation**: \[ \frac{hc}{100 \times 10^{-9}} - 4\phi = \frac{hc}{250 \times 10^{-9}} - \phi \] Rearranging gives: \[ \frac{hc}{100 \times 10^{-9}} - \frac{hc}{250 \times 10^{-9}} = 3\phi \] 9. **Finding a Common Denominator**: The common denominator for \( 100 \) and \( 250 \) is \( 500 \): \[ \frac{5hc - 2hc}{500 \times 10^{-9}} = 3\phi \] This simplifies to: \[ \frac{3hc}{500 \times 10^{-9}} = 3\phi \] 10. **Solving for Work Function \( \phi \)**: Dividing both sides by 3: \[ \phi = \frac{hc}{500 \times 10^{-9}} \] 11. **Final Expression**: \[ \phi = \frac{hc}{500 \times 10^{-9}} = \frac{hc}{5 \times 10^{-7}} \]

To find the work function of the metal when illuminated by light of wavelengths 400 nm and 250 nm, we can use the photoelectric effect equation derived from Einstein's photoelectric equation: 1. **Understanding the Problem**: - We have two wavelengths: \( \lambda_1 = 400 \, \text{nm} \) and \( \lambda_2 = 250 \, \text{nm} \). - The maximum velocities of the photoelectrons are \( v_1 = v \) for \( \lambda_1 \) and \( v_2 = 2v \) for \( \lambda_2 \). 2. **Using the Photoelectric Equation**: The kinetic energy of the emitted photoelectrons can be expressed as: ...
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