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find kinetic energy, electrostatic potential energy and total
. energy of single electron in 2nd excited state of `Li^(+2)` atom.

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To find the kinetic energy, electrostatic potential energy, and total energy of a single electron in the second excited state of the `Li^(+2)` atom, we can follow these steps: ### Step 1: Identify the quantum numbers The second excited state corresponds to the principal quantum number \( n = 3 \). For lithium, the atomic number \( Z = 3 \). ### Step 2: Calculate the total energy The formula for the energy of an electron in a hydrogen-like atom is given by: \[ E = -\frac{13.6 Z^2}{n^2} \] Substituting the values for lithium: \[ E = -\frac{13.6 \times 3^2}{3^2} \] Calculating this gives: \[ E = -\frac{13.6 \times 9}{9} = -13.6 \text{ eV} \] ### Step 3: Calculate the kinetic energy The kinetic energy \( K \) of the electron in a hydrogen-like atom is equal to the absolute value of the total energy: \[ K = |E| = 13.6 \text{ eV} \] ### Step 4: Calculate the electrostatic potential energy The electrostatic potential energy \( U \) is given by: \[ U = 2E \] Substituting the value of \( E \): \[ U = 2 \times (-13.6) = -27.2 \text{ eV} \] ### Step 5: Calculate the total energy The total energy \( E_{total} \) is simply the sum of kinetic energy and potential energy: \[ E_{total} = K + U \] Substituting the values: \[ E_{total} = 13.6 + (-27.2) = -13.6 \text{ eV} \] ### Summary of Results - Kinetic Energy \( K = 13.6 \text{ eV} \) - Electrostatic Potential Energy \( U = -27.2 \text{ eV} \) - Total Energy \( E_{total} = -13.6 \text{ eV} \)

To find the kinetic energy, electrostatic potential energy, and total energy of a single electron in the second excited state of the `Li^(+2)` atom, we can follow these steps: ### Step 1: Identify the quantum numbers The second excited state corresponds to the principal quantum number \( n = 3 \). For lithium, the atomic number \( Z = 3 \). ### Step 2: Calculate the total energy The formula for the energy of an electron in a hydrogen-like atom is given by: ...
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