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Lights of wavelenths lambda(1)=340nm and...

Lights of wavelenths `lambda_(1)=340nm` and `lambda_(2)=540nm` are incident on a metallic surface. If the ratio of the maximum speeds of electrons ejected is 2, the work function of the metal is

A

2 eV

B

1.8 eV

C

1 eV

D

1.5 eV

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The correct Answer is:
To solve the problem, we need to find the work function of the metal given the wavelengths of incident light and the ratio of the maximum speeds of the ejected electrons. ### Step-by-Step Solution: 1. **Identify Given Values**: - Wavelengths of light: - \( \lambda_1 = 340 \, \text{nm} \) - \( \lambda_2 = 540 \, \text{nm} \) - Ratio of maximum speeds of ejected electrons: - \( \frac{v_1}{v_2} = 2 \) 2. **Use the Photoelectric Equation**: The energy of the photons can be expressed using the equation: \[ E = \frac{hc}{\lambda} \] where \( h \) is Planck's constant and \( c \) is the speed of light. 3. **Write the Energy Equations for Each Wavelength**: For the first wavelength \( \lambda_1 \): \[ E_1 = \frac{hc}{\lambda_1} = \frac{hc}{340 \, \text{nm}} \] For the second wavelength \( \lambda_2 \): \[ E_2 = \frac{hc}{\lambda_2} = \frac{hc}{540 \, \text{nm}} \] 4. **Apply the Photoelectric Effect Equation**: The energy of the incident photon is used to overcome the work function \( \phi \) and provide kinetic energy to the ejected electron: \[ E_1 = \phi + KE_1 \quad \text{and} \quad E_2 = \phi + KE_2 \] where \( KE = \frac{1}{2}mv^2 \). 5. **Express Kinetic Energy in Terms of Speed**: From the ratio of speeds: \[ KE_1 = \frac{1}{2}mv_1^2 \quad \text{and} \quad KE_2 = \frac{1}{2}mv_2^2 \] Given \( \frac{v_1}{v_2} = 2 \), we can express \( v_1 \) in terms of \( v_2 \): \[ v_1 = 2v_2 \implies KE_1 = \frac{1}{2}m(2v_2)^2 = 2mv_2^2 = 4KE_2 \] 6. **Set Up the Equations**: Substituting \( KE_1 \) and \( KE_2 \) into the energy equations: \[ \frac{hc}{340} = \phi + 4KE_2 \quad \text{(1)} \] \[ \frac{hc}{540} = \phi + KE_2 \quad \text{(2)} \] 7. **Eliminate Work Function \( \phi \)**: From equation (2): \[ \phi = \frac{hc}{540} - KE_2 \] Substitute \( \phi \) into equation (1): \[ \frac{hc}{340} = \left(\frac{hc}{540} - KE_2\right) + 4KE_2 \] Simplifying gives: \[ \frac{hc}{340} = \frac{hc}{540} + 3KE_2 \] 8. **Solve for \( KE_2 \)**: Rearranging: \[ 3KE_2 = \frac{hc}{340} - \frac{hc}{540} \] Finding a common denominator (which is \( 340 \times 540 \)): \[ 3KE_2 = \frac{hc(540 - 340)}{340 \times 540} \] \[ 3KE_2 = \frac{hc(200)}{340 \times 540} \] \[ KE_2 = \frac{hc(200)}{3 \times 340 \times 540} \] 9. **Substitute Back to Find Work Function**: Substitute \( KE_2 \) back into the equation for \( \phi \): \[ \phi = \frac{hc}{540} - \frac{hc(200)}{3 \times 340 \times 540} \] Simplifying gives the work function in terms of \( h \) and \( c \). 10. **Calculate Numerical Value**: Using \( h = 6.626 \times 10^{-34} \, \text{Js} \) and \( c = 3 \times 10^8 \, \text{m/s} \), convert nm to meters, and calculate \( \phi \). ### Final Answer: After performing the calculations, we find that the work function \( \phi \) is approximately \( 1.8 \, \text{eV} \).
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