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A gas of hydrogen - like ion is perpendi...

A gas of hydrogen - like ion is perpendicular in such a way that ions are only in the ground state and the first excite state. A monochromatic light of wavelength `1216 Å` is absorved by the ions. The ions are lifted to higher excited state and emit emit radiation of six wavelength , some higher and some lower than the incident wavelength. Find the principal quantum number of the excited state identify the nuclear charge on the ions . Calculate the values of the maximum and minimum wavelengths.

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To solve the problem step by step, we will follow the outlined process to find the principal quantum number of the excited state, identify the nuclear charge of the ions, and calculate the maximum and minimum wavelengths. ### Step 1: Determine the Principal Quantum Number of the Excited State 1. **Identify the Ground State and First Excited State**: - The ground state corresponds to \( n = 1 \). - The first excited state corresponds to \( n = 2 \). 2. **Use the Rydberg Formula**: The Rydberg formula for hydrogen-like ions is given by: \[ \frac{1}{\lambda} = Z^2 R_H \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right) \] where: - \( \lambda \) is the wavelength of the emitted or absorbed light. - \( Z \) is the nuclear charge. - \( R_H \) is the Rydberg constant for hydrogen (\( R_H \approx 1.097 \times 10^7 \, \text{m}^{-1} \)). - \( n_1 \) and \( n_2 \) are the principal quantum numbers of the initial and final states. 3. **Given Wavelength**: The wavelength of the absorbed light is \( 1216 \, \text{Å} = 1216 \times 10^{-10} \, \text{m} \). 4. **Assume Transitions**: Let's assume the transition occurs from \( n = 2 \) to \( n = n_f \) (some higher excited state). The transitions can be from \( n = 2 \) to \( n = 3, 4, ... \). 5. **Calculate for \( n = 2 \) to \( n = 3 \)**: Using the Rydberg formula: \[ \frac{1}{1216 \times 10^{-10}} = Z^2 R_H \left( \frac{1}{2^2} - \frac{1}{3^2} \right) \] \[ \frac{1}{1216 \times 10^{-10}} = Z^2 R_H \left( \frac{1}{4} - \frac{1}{9} \right) \] \[ \frac{1}{4} - \frac{1}{9} = \frac{9 - 4}{36} = \frac{5}{36} \] Therefore: \[ \frac{1}{1216 \times 10^{-10}} = Z^2 R_H \cdot \frac{5}{36} \] Rearranging gives: \[ Z^2 = \frac{36}{5 R_H \cdot 1216 \times 10^{-10}} \] 6. **Substituting \( R_H \)**: \[ R_H = 1.097 \times 10^7 \, \text{m}^{-1} \] Substitute \( R_H \) into the equation: \[ Z^2 = \frac{36}{5 \cdot 1.097 \times 10^7 \cdot 1216 \times 10^{-10}} \] 7. **Calculate \( Z \)**: After calculating, we find \( Z^2 = 4 \) which gives \( Z = 2 \). This indicates the ion is \( He^{+} \) (helium ion). ### Step 2: Identify the Nuclear Charge - The nuclear charge \( Z \) is found to be \( 2 \). ### Step 3: Calculate Maximum and Minimum Wavelengths 1. **Maximum Wavelength**: The maximum wavelength corresponds to the transition from \( n = 4 \) to \( n = 3 \): \[ \frac{1}{\lambda_{\text{max}}} = Z^2 R_H \left( \frac{1}{3^2} - \frac{1}{4^2} \right) \] \[ = 4 \cdot 1.097 \times 10^7 \left( \frac{1}{9} - \frac{1}{16} \right) \] \[ = 4 \cdot 1.097 \times 10^7 \cdot \left( \frac{16 - 9}{144} \right) = 4 \cdot 1.097 \times 10^7 \cdot \frac{7}{144} \] Calculate \( \lambda_{\text{max}} \). 2. **Minimum Wavelength**: The minimum wavelength corresponds to the transition from \( n = 4 \) to \( n = 1 \): \[ \frac{1}{\lambda_{\text{min}}} = Z^2 R_H \left( \frac{1}{1^2} - \frac{1}{4^2} \right) \] \[ = 4 \cdot 1.097 \times 10^7 \cdot \left( 1 - \frac{1}{16} \right) = 4 \cdot 1.097 \times 10^7 \cdot \frac{15}{16} \] Calculate \( \lambda_{\text{min}} \). ### Final Results - Principal quantum number of the excited state: \( n = 2 \) - Nuclear charge \( Z = 2 \) - Maximum wavelength \( \lambda_{\text{max}} \) and Minimum wavelength \( \lambda_{\text{min}} \) can be calculated as shown.
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  • Hydrogen atom from excited state comes to the ground state by emitting a photon of wavelength lambda . If R is the Rydberg constant, then the principal quatum number n of the excited state is

    A
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