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In a black body radiation at certain tem...

In a black body radiation at certain temperature `T_1` the wave length having maximum intensity of radiation equals `9000A^@` . When the temperature is increased from `T_1 "to" T_2` the total radiation increases 16 times. The peak radiation at `T_2` is found to be capable of ejecting photoelectrons.
The maximum kinetic energy of photoelectrons is the same as the energy of photon that one gets when one of electron in the M -shall of hydrogen atom jumps to L-shell the work function of the metal will be

A

0.88 eV

B

1.5 eV

C

2.0 eV

D

1.2 eV

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To solve the problem step by step, we will follow the reasoning laid out in the video transcript. ### Step 1: Understanding the relationship between temperatures and radiation According to Stefan's law, the radiant heat energy emitted from a unit area in one second is given by: \[ E = \sigma T^4 \] where \( E \) is the radiant energy, \( \sigma \) is the Stefan-Boltzmann constant, and \( T \) is the absolute temperature. Let: - \( E_1 = \sigma T_1^4 \) (at temperature \( T_1 \)) - \( E_2 = \sigma T_2^4 \) (at temperature \( T_2 \)) Given that the total radiation increases 16 times when the temperature changes from \( T_1 \) to \( T_2 \), we have: \[ E_2 = 16 E_1 \] ### Step 2: Setting up the equations Substituting the expressions for \( E_1 \) and \( E_2 \): \[ \sigma T_2^4 = 16 \sigma T_1^4 \] We can cancel \( \sigma \) from both sides: \[ T_2^4 = 16 T_1^4 \] Taking the fourth root of both sides: \[ T_2 = 2 T_1 \] ### Step 3: Using Wien's Law to find the new wavelength Wien's Law states: \[ \lambda_1 T_1 = \lambda_2 T_2 \] Given that \( \lambda_1 = 9000 \, \text{Å} \) and substituting \( T_2 = 2 T_1 \): \[ 9000 \, \text{Å} \cdot T_1 = \lambda_2 \cdot (2 T_1) \] Cancelling \( T_1 \) from both sides: \[ \lambda_2 = \frac{9000 \, \text{Å}}{2} = 4500 \, \text{Å} \] ### Step 4: Finding the maximum kinetic energy of photoelectrons The maximum kinetic energy of the photoelectrons is equal to the energy of the photon emitted when an electron transitions from the M-shell (n=3) to the L-shell (n=2) in a hydrogen atom. The energy difference is given by: \[ KE = -13.6 \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right) \] where \( n_1 = 2 \) and \( n_2 = 3 \): \[ KE = -13.6 \left( \frac{1}{2^2} - \frac{1}{3^2} \right) \] \[ KE = -13.6 \left( \frac{1}{4} - \frac{1}{9} \right) \] Calculating the fractions: \[ KE = -13.6 \left( \frac{9 - 4}{36} \right) = -13.6 \left( \frac{5}{36} \right) \] \[ KE = -13.6 \times 0.1389 \approx 1.89 \, \text{eV} \] ### Step 5: Finding the work function of the metal The work function \( \phi \) of the metal can be found using the equation: \[ \phi = E - KE \] where \( E \) is the energy of the photon corresponding to the wavelength \( \lambda_2 \): \[ E = \frac{hc}{\lambda_2} \] Substituting \( h = 6.626 \times 10^{-34} \, \text{Js} \) and \( c = 3 \times 10^8 \, \text{m/s} \): Convert \( \lambda_2 = 4500 \, \text{Å} = 4500 \times 10^{-10} \, \text{m} \): \[ E = \frac{(6.626 \times 10^{-34})(3 \times 10^8)}{4500 \times 10^{-10}} \] Calculating: \[ E \approx 2.75 \, \text{eV} \] Now, substituting back to find the work function: \[ \phi = 2.75 \, \text{eV} - 1.89 \, \text{eV} = 0.86 \, \text{eV} \] ### Final Answer The work function of the metal is approximately: \[ \phi \approx 0.88 \, \text{eV} \]
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