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If the I excitation potential of a hypot...

If the I excitation potential of a hypothetical H-like is 162 V, then the value of II excitation energy is about :

A

192 eV

B

30 eV

C

216 eV

D

40.5 eV

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To solve the problem of finding the second excitation energy of a hypothetical hydrogen-like atom given that the first excitation potential is 162 V, we can follow these steps: ### Step 1: Understand the Formula for Excitation Potential The excitation potential for the first excitation level of a hydrogen-like atom is given by the formula: \[ E_1 = 10.2 \times Z^2 \] where \(E_1\) is the first excitation potential and \(Z\) is the atomic number. ### Step 2: Substitute the Given Value We know from the problem that \(E_1 = 162 \, \text{V}\). We can set up the equation: \[ 162 = 10.2 \times Z^2 \] ### Step 3: Solve for \(Z^2\) To find \(Z^2\), we rearrange the equation: \[ Z^2 = \frac{162}{10.2} \] Calculating this gives: \[ Z^2 = 15.8824 \] ### Step 4: Use the Formula for Second Excitation Energy The formula for the second excitation energy \(E_2\) for hydrogen-like species is: \[ E_2 = 12.09 \times Z^2 \] ### Step 5: Substitute \(Z^2\) into the Second Excitation Energy Formula Now, we substitute the value of \(Z^2\) into the equation: \[ E_2 = 12.09 \times 15.8824 \] ### Step 6: Calculate \(E_2\) Performing the multiplication: \[ E_2 \approx 192.01 \, \text{eV} \] ### Step 7: Round to the Nearest Whole Number The nearest whole number to 192.01 is: \[ E_2 \approx 192 \, \text{eV} \] ### Conclusion Thus, the value of the second excitation energy is approximately **192 eV**.

To solve the problem of finding the second excitation energy of a hypothetical hydrogen-like atom given that the first excitation potential is 162 V, we can follow these steps: ### Step 1: Understand the Formula for Excitation Potential The excitation potential for the first excitation level of a hydrogen-like atom is given by the formula: \[ E_1 = 10.2 \times Z^2 \] where \(E_1\) is the first excitation potential and \(Z\) is the atomic number. ...
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