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An electron in Bohr's hydrogen atom has ...

An electron in Bohr's hydrogen atom has an energy of -3.4 eV. The angular momentum of the electron is

A

`(h)/(pi)`

B

`(h)/(2pi)`

C

`(nh)/(2pi)`(n is an integer)

D

`(2h)/(pi)`

Text Solution

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The correct Answer is:
To find the angular momentum of an electron in a hydrogen atom with a given energy of -3.4 eV, we can follow these steps: ### Step 1: Understand the energy formula in Bohr's model In Bohr's model of the hydrogen atom, the energy of an electron in the nth orbit is given by the formula: \[ E = -\frac{13.6 \, \text{eV}}{n^2} \] where \( E \) is the energy of the electron and \( n \) is the principal quantum number (orbit number). ### Step 2: Set up the equation with the given energy Given that the energy \( E = -3.4 \, \text{eV} \), we can set up the equation: \[ -3.4 = -\frac{13.6}{n^2} \] ### Step 3: Solve for \( n^2 \) Removing the negative signs from both sides gives: \[ 3.4 = \frac{13.6}{n^2} \] Now, rearranging the equation to solve for \( n^2 \): \[ n^2 = \frac{13.6}{3.4} \] ### Step 4: Calculate \( n^2 \) Calculating the right side: \[ n^2 = \frac{13.6}{3.4} = 4 \] Taking the square root gives: \[ n = 2 \] ### Step 5: Use the angular momentum formula According to Bohr's model, the angular momentum \( L \) of the electron in the nth orbit is given by: \[ L = n \cdot \frac{h}{2\pi} \] Substituting the value of \( n \): \[ L = 2 \cdot \frac{h}{2\pi} \] ### Step 6: Simplify the expression Simplifying the expression: \[ L = \frac{h}{\pi} \] ### Final Answer Thus, the angular momentum of the electron is: \[ L = \frac{h}{\pi} \] ---

To find the angular momentum of an electron in a hydrogen atom with a given energy of -3.4 eV, we can follow these steps: ### Step 1: Understand the energy formula in Bohr's model In Bohr's model of the hydrogen atom, the energy of an electron in the nth orbit is given by the formula: \[ E = -\frac{13.6 \, \text{eV}}{n^2} \] where \( E \) is the energy of the electron and \( n \) is the principal quantum number (orbit number). ...
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