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Total energy of an electron in nth stati...

Total energy of an electron in nth stationary orcit of hydrogen atom can be obtained by

A

`E_n = 13.6/ n^2 eV`

B

`E_n = -13.6/ n^2 eV`

C

`E_n = -13.6/ n^2 eV`

D

`E_n = 13.6 x n^2 eV`

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The correct Answer is:
To find the total energy of an electron in the nth stationary orbit of a hydrogen atom, we can follow these steps: ### Step-by-Step Solution: 1. **Understanding the Forces**: The electron in a hydrogen atom moves in a circular orbit around the nucleus (proton). The centripetal force required for this circular motion is provided by the electrostatic force of attraction between the electron and the proton. 2. **Centripetal Force and Electrostatic Force**: - The centripetal force can be expressed as: \[ F_c = \frac{mv^2}{r_n} \] where \( m \) is the mass of the electron, \( v \) is its velocity, and \( r_n \) is the radius of the nth orbit. - The electrostatic force between the electron and the proton is given by Coulomb's law: \[ F_e = \frac{k \cdot e^2}{r_n^2} \] where \( k \) is Coulomb's constant, and \( e \) is the charge of the electron. 3. **Setting the Forces Equal**: For the electron to remain in a stable orbit, the centripetal force must equal the electrostatic force: \[ \frac{mv^2}{r_n} = \frac{k \cdot e^2}{r_n^2} \] Rearranging gives: \[ mv^2 = \frac{k \cdot e^2}{r_n} \] 4. **Angular Momentum Quantization**: According to Bohr's model, the angular momentum of the electron is quantized: \[ mvr_n = n\frac{h}{2\pi} \] where \( n \) is a positive integer (the principal quantum number) and \( h \) is Planck's constant. 5. **Finding the Radius of the nth Orbit**: By solving the equations for \( r_n \) and substituting the expression for \( v \), we find: \[ r_n = \frac{n^2 h^2}{4\pi^2 k e^2 m} \] This can be simplified to: \[ r_n = 0.529 \frac{n^2}{Z} \text{ Å} \] for hydrogen, where \( Z = 1 \). 6. **Kinetic Energy (KE)**: The kinetic energy of the electron in the nth orbit can be expressed as: \[ KE = \frac{1}{2} mv^2 \] Using the earlier relationship, we find: \[ KE = \frac{k \cdot e^2}{2r_n} \] 7. **Potential Energy (PE)**: The potential energy of the electron in the nth orbit is given by: \[ PE = -\frac{k \cdot e^2}{r_n} \] 8. **Total Energy (E)**: The total energy of the electron is the sum of its kinetic and potential energies: \[ E_n = KE + PE = \frac{k \cdot e^2}{2r_n} - \frac{k \cdot e^2}{r_n} = -\frac{k \cdot e^2}{2r_n} \] 9. **Substituting for Hydrogen**: For hydrogen (\( Z = 1 \)), we substitute the values to find: \[ E_n = -\frac{13.6 \, \text{eV}}{n^2} \] ### Final Result: Thus, the total energy of an electron in the nth stationary orbit of a hydrogen atom is: \[ E_n = -\frac{13.6}{n^2} \text{ eV} \]
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