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 energy of an electron in first Bohr orbit of H-atom is $-13.6$ eV. The magnitude of energy value of electron in the first excited state of Be$^{3+}$ is _____ eV (nearest integer value)
Correct statements for an element with atomic number 9 are
A. There can be 5 electrons for which $ m_s = +\frac{1}{2} $ and 4 electrons for which $ m_s = -\frac{1}{2} $
B. There is only one electron in $ p_z $ orbital.
C. The last electron goes to orbital with $ n = 2 $ and $ l = 1 $.
D. The sum of angular nodes of all the atomic orbitals is 1.
Choose the correct answer from the options given below:
Which of the following is/are correct with respect to the energy of atomic orbitals of a hydrogen atom?
(A) \( 1s<2s<2p<3d<4s \)
(B) \( 1s<2s = 2p<3s = 3p \)
(C) \( 1s<2s<2p<3s<3p \)
(D) \( 1s<2s<4s<3d \)
Choose the correct answer from the options given below:
The term independent of $ x $ in the expansion of $$ \left( \frac{x + 1}{x^{3/2} + 1 - \sqrt{x}} \cdot \frac{x + 1}{x - \sqrt{x}} \right)^{10} $$ for $ x>1 $ is:

Two cells of emf 1V and 2V and internal resistance 2 \( \Omega \) and 1 \( \Omega \), respectively, are connected in series with an external resistance of 6 \( \Omega \). The total current in the circuit is \( I_1 \). Now the same two cells in parallel configuration are connected to the same external resistance. In this case, the total current drawn is \( I_2 \). The value of \( \left( \frac{I_1}{I_2} \right) \) is \( \frac{x}{3} \). The value of x is 1cm.
If $ \theta \in [-2\pi,\ 2\pi] $, then the number of solutions of $$ 2\sqrt{2} \cos^2\theta + (2 - \sqrt{6}) \cos\theta - \sqrt{3} = 0 $$ is: