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Monochromatic radiation emitted when ele...

Monochromatic radiation emitted when electron on hydrogen atom jumps from first excited to the ground state irradiates a photosensitive material. The stopping potential is measured to be `3.57V`. The threshold frequency of the material is

A

`4 xx 10^(15)` Hz

B

`5 xx 10^(15)`Hz

C

`1.6 xx 10^(15)`Hz

D

`2.5 xx 10^(15)`Hz

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to find the threshold frequency of the photosensitive material when an electron in a hydrogen atom transitions from the first excited state to the ground state. Here's a step-by-step solution: ### Step 1: Determine the energy levels of the hydrogen atom The energy levels of a hydrogen atom are given by the formula: \[ E_n = -\frac{13.6 \, \text{eV}}{n^2} \] where \( n \) is the principal quantum number. ### Step 2: Calculate the energy of the first excited state (n=2) For the first excited state (n=2): \[ E_2 = -\frac{13.6 \, \text{eV}}{2^2} = -\frac{13.6 \, \text{eV}}{4} = -3.4 \, \text{eV} \] ### Step 3: Calculate the energy of the ground state (n=1) For the ground state (n=1): \[ E_1 = -\frac{13.6 \, \text{eV}}{1^2} = -13.6 \, \text{eV} \] ### Step 4: Calculate the energy difference (photon energy) The energy difference when the electron jumps from n=2 to n=1 is: \[ E = E_1 - E_2 = (-13.6 \, \text{eV}) - (-3.4 \, \text{eV}) = -13.6 + 3.4 = -10.2 \, \text{eV} \] Thus, the energy of the emitted photon is: \[ E = 10.2 \, \text{eV} \] ### Step 5: Relate stopping potential to photon energy The stopping potential \( V_0 \) is given as 3.57 V. The energy of the photon can also be expressed in terms of the stopping potential: \[ E = eV_0 \] where \( e \) is the charge of an electron (approximately \( 1.6 \times 10^{-19} \, \text{C} \)). Therefore: \[ E = 3.57 \, \text{eV} \] ### Step 6: Calculate the work function (Φ) Using the relationship between photon energy, stopping potential, and work function: \[ E = eV_0 + \Phi \] Substituting the values: \[ 10.2 \, \text{eV} = 3.57 \, \text{eV} + \Phi \] Solving for \( \Phi \): \[ \Phi = 10.2 \, \text{eV} - 3.57 \, \text{eV} = 6.63 \, \text{eV} \] ### Step 7: Calculate the threshold frequency (ν₀) The work function is related to the threshold frequency by the equation: \[ \Phi = h\nu_0 \] where \( h \) is Planck's constant (\( 6.63 \times 10^{-34} \, \text{Js} \)). We can convert the work function from eV to joules: \[ \Phi = 6.63 \, \text{eV} \times 1.6 \times 10^{-19} \, \text{J/eV} = 1.0608 \times 10^{-18} \, \text{J} \] Now, we can solve for \( \nu_0 \): \[ \nu_0 = \frac{\Phi}{h} = \frac{1.0608 \times 10^{-18} \, \text{J}}{6.63 \times 10^{-34} \, \text{Js}} \approx 1.6 \times 10^{15} \, \text{Hz} \] ### Final Answer The threshold frequency of the material is: \[ \nu_0 \approx 1.6 \times 10^{15} \, \text{Hz} \] ---
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