The orbital angular momentum of an electron in an atom is given by the formula: \[ L = \sqrt{l(l+1)} \frac{h}{2\pi} = \sqrt{l(l+1)} \hbar \] where \( l \) is the azimuthal quantum number (also known as the orbital angular momentum quantum number), and \( h \) is Planck's constant, with \( \hbar = \frac{h}{2\pi} \) being the reduced Planck constant.
For a '2s' orbital, the principal quantum number \( n = 2 \), and for an 's' orbital, the azimuthal quantum number \( l = 0 \). Substituting \( l = 0 \) into the formula for orbital angular momentum: \[ L_{2s} = \sqrt{0(0+1)} \frac{h}{2\pi} = \sqrt{0} \frac{h}{2\pi} = 0 \] So, the orbital angular momentum for an electron in a 2s orbital is 0. For a '2p' orbital, the principal quantum number \( n = 2 \), and for a 'p' orbital, the azimuthal quantum number \( l = 1 \). Substituting \( l = 1 \) into the formula for orbital angular momentum: \[ L_{2p} = \sqrt{1(1+1)} \frac{h}{2\pi} = \sqrt{1(2)} \frac{h}{2\pi} = \sqrt{2} \frac{h}{2\pi} \] So, the orbital angular momentum for an electron in a 2p orbital is \( \sqrt{2} \frac{h}{2\pi} \). The orbital angular momentum values for electrons in '2s' and '2p' orbitals are 0 and \( \sqrt{2} \frac{h}{2\pi} \) respectively.
This corresponds to option (4).
The orbital angular momentum of an electron in an atomic orbital is given by the formula:
\(L = \sqrt{l(l+1)} \frac{h}{2\pi}\)
where:
The azimuthal quantum number \(l\) determines the subshell of the electron:
Now, calculate the orbital angular momentum for:
Since \(l = 0\)
\(L = \sqrt{0(0+1)} \frac{h}{2\pi} = 0\)
Since \(l = 1\)
\(L = \sqrt{1(1+1)} \frac{h}{2\pi} = \sqrt{2} \frac{h}{2\pi}\)
Therefore, for electrons in 2s and 2p orbitals, the orbital angular momentum values are 0 and \(\sqrt{2} \frac{h}{2\pi}\) respectively.
So, the correct answer is: 0 and \(\sqrt{2} \frac{h}{2\pi}\).
The figures below show:
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