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Light of wavelength 0.6mum from a sodium...

Light of wavelength `0.6mum` from a sodium lamp falls on a photocell and causes the emission of photoelectrons for which the stopping potential is 0.5V. With light of wavelength `0.4mum` from a murcury vapor lamp, the stopping potential is `1.5V`. Then, the work function [in electron volts] of the photocell surface is

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To find the work function (W₀) of the photocell surface, we will use the photoelectric equation: \[ E - W_0 = eV_s \] Where: - \( E \) is the energy of the incident photons, - \( W_0 \) is the work function, - \( e \) is the charge of an electron, - \( V_s \) is the stopping potential. The energy of the photons can be calculated using the formula: \[ E = \frac{hc}{\lambda} \] Where: - \( h \) is Planck's constant (\( 6.626 \times 10^{-34} \, \text{Js} \)), - \( c \) is the speed of light (\( 3 \times 10^8 \, \text{m/s} \)), - \( \lambda \) is the wavelength of the light. ### Step 1: Calculate the energy for the sodium lamp (λ = 0.6 μm) Convert the wavelength from micrometers to meters: \[ \lambda_1 = 0.6 \, \mu m = 0.6 \times 10^{-6} \, m \] Now, calculate the energy \( E_1 \): \[ E_1 = \frac{hc}{\lambda_1} = \frac{(6.626 \times 10^{-34} \, \text{Js})(3 \times 10^8 \, \text{m/s})}{0.6 \times 10^{-6} \, m} \] Calculating this gives: \[ E_1 = \frac{1.9878 \times 10^{-25}}{0.6 \times 10^{-6}} = 3.313 \times 10^{-19} \, J \] To convert this energy to electron volts (1 eV = \( 1.6 \times 10^{-19} \, J \)): \[ E_1 = \frac{3.313 \times 10^{-19}}{1.6 \times 10^{-19}} \approx 2.07 \, eV \] ### Step 2: Use the stopping potential for sodium lamp Given the stopping potential \( V_s = 0.5 \, V \): Using the photoelectric equation: \[ E_1 - W_0 = eV_s \] Substituting the values: \[ 2.07 \, eV - W_0 = 0.5 \, V \] Rearranging gives: \[ W_0 = 2.07 \, eV - 0.5 \, V = 1.57 \, eV \] ### Step 3: Calculate the energy for the mercury lamp (λ = 0.4 μm) Convert the wavelength: \[ \lambda_2 = 0.4 \, \mu m = 0.4 \times 10^{-6} \, m \] Calculate the energy \( E_2 \): \[ E_2 = \frac{hc}{\lambda_2} = \frac{(6.626 \times 10^{-34} \, \text{Js})(3 \times 10^8 \, \text{m/s})}{0.4 \times 10^{-6} \, m} \] Calculating this gives: \[ E_2 = \frac{1.9878 \times 10^{-25}}{0.4 \times 10^{-6}} = 4.9695 \times 10^{-19} \, J \] Convert to electron volts: \[ E_2 = \frac{4.9695 \times 10^{-19}}{1.6 \times 10^{-19}} \approx 3.10 \, eV \] ### Step 4: Use the stopping potential for mercury lamp Given the stopping potential \( V_s = 1.5 \, V \): Using the photoelectric equation: \[ E_2 - W_0 = eV_s \] Substituting the values: \[ 3.10 \, eV - W_0 = 1.5 \, V \] Rearranging gives: \[ W_0 = 3.10 \, eV - 1.5 \, V = 1.60 \, eV \] ### Conclusion The work function \( W_0 \) of the photocell surface is approximately \( 1.60 \, eV \).
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