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If in a photoelectric cell , the wavelen...

If in a photoelectric cell , the wavelength of incident light is changed from 4000 Å to 3000 Å then change in stopping potential will be

A

0.66 V

B

1.03 V

C

0.33 V

D

0,49 V

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To solve the problem of finding the change in stopping potential when the wavelength of incident light is changed from 4000 Å to 3000 Å in a photoelectric cell, we can follow these steps: ### Step 1: Understand the Photoelectric Equation The photoelectric effect is described by Einstein's photoelectric equation: \[ \frac{hc}{\lambda} - \phi = eV_0 \] where: - \( h \) = Planck's constant (\( 6.63 \times 10^{-34} \, \text{Js} \)) - \( c \) = speed of light (\( 3 \times 10^8 \, \text{m/s} \)) - \( \lambda \) = wavelength of the incident light - \( \phi \) = work function of the material - \( e \) = charge of an electron (\( 1.6 \times 10^{-19} \, \text{C} \)) - \( V_0 \) = stopping potential ### Step 2: Set Up the Equations for Two Wavelengths Let: - \( \lambda_1 = 4000 \, \text{Å} = 4000 \times 10^{-10} \, \text{m} \) - \( \lambda_2 = 3000 \, \text{Å} = 3000 \times 10^{-10} \, \text{m} \) Using the photoelectric equation for both wavelengths: 1. For \( \lambda_1 \): \[ \frac{hc}{\lambda_1} - \phi = eV_{01} \] 2. For \( \lambda_2 \): \[ \frac{hc}{\lambda_2} - \phi = eV_{02} \] ### Step 3: Subtract the Two Equations Subtract the second equation from the first: \[ \left(\frac{hc}{\lambda_1} - \phi\right) - \left(\frac{hc}{\lambda_2} - \phi\right) = eV_{01} - eV_{02} \] This simplifies to: \[ \frac{hc}{\lambda_1} - \frac{hc}{\lambda_2} = e(V_{01} - V_{02}) \] ### Step 4: Rearrange for Change in Stopping Potential Rearranging gives us: \[ V_{01} - V_{02} = \frac{hc}{e} \left(\frac{1}{\lambda_1} - \frac{1}{\lambda_2}\right) \] ### Step 5: Substitute Values Now substitute the known values: - \( h = 6.63 \times 10^{-34} \, \text{Js} \) - \( c = 3 \times 10^8 \, \text{m/s} \) - \( e = 1.6 \times 10^{-19} \, \text{C} \) - \( \lambda_1 = 4000 \times 10^{-10} \, \text{m} \) - \( \lambda_2 = 3000 \times 10^{-10} \, \text{m} \) Calculating: \[ V_{01} - V_{02} = \frac{(6.63 \times 10^{-34})(3 \times 10^8)}{1.6 \times 10^{-19}} \left(\frac{1}{4000 \times 10^{-10}} - \frac{1}{3000 \times 10^{-10}}\right) \] ### Step 6: Calculate the Values Calculate \( \frac{hc}{e} \): \[ \frac{(6.63 \times 10^{-34})(3 \times 10^8)}{1.6 \times 10^{-19}} \approx 1.24 \, \text{V} \] Now calculate \( \left(\frac{1}{4000 \times 10^{-10}} - \frac{1}{3000 \times 10^{-10}}\right) \): \[ \frac{1}{4000 \times 10^{-10}} - \frac{1}{3000 \times 10^{-10}} = \frac{3 - 4}{12000} = -\frac{1}{12000} \, \text{m}^{-1} \] ### Step 7: Final Calculation Putting it all together: \[ V_{01} - V_{02} = 1.24 \times -\frac{1}{12000} \approx -0.103 \, \text{V} \approx -1.03 \, \text{V} \] Thus, the change in stopping potential is: \[ V_{02} - V_{01} = 1.03 \, \text{V} \] ### Conclusion The change in stopping potential when the wavelength is changed from 4000 Å to 3000 Å is approximately \( 1.03 \, \text{V} \).
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