Angular Momentum of Electron - De Broglie's Explanation, FAQs

Angular Momentum of Electron - De Broglie's Explanation, FAQs

Vishal kumarUpdated on 02 Jul 2025, 04:45 PM IST

Introduction:
The rotating equivalent of linear momentum is angular momentum in physics. Because it is a preserved measure, the total angular momentum of a sealed system remains constant. It is a significant quantity in physics. Angular momentum of electron formula is mvr or nh/2. In this article we will study in detail about angular momentum of an electron, quantisation of angular momentum, property of an electron moving in a circular orbit and orbital angular momentum of an electron. Also, the quantised meaning in Tamil is அளவிடப்பட்டது.

Angular Momentum of Electron - De Broglie's Explanation, FAQs
Angular Momentum of Electron

Electron spin:

The spinning electron was successful in describing not only fine structure and the strange Zeeman Effect, but also other atomic phenomena.

The Bohr Sommerfeld quantum theory of elliptic orbits with relativity correction was in fair numerical agreement with the observed fine structure of hydrogen spectral lines. It however, suffered from two main drawbacks or downsides:

  1. Firstly, Summerfield's relativistic explanation could not be applied for the spectral lines of atoms other than hydrogen. Alkali atoms' spectral lines, for example, are doublets with two near fine-structure components. The (single) optical electron in alkali atoms moves in a Bohr-like orbit with a large radius and low velocity. Therefore, the relativity effect would be too small to account for the large (compared with hydrogen) Fine-structure splitting observed in alkali lines.
  2. Secondly, the simple quantum theory failed to explain the anomalous Zeeman Effect, that is, the splitting of atomic spectral lines into four, six or more components when the light source was placed in an external magnetic field.

In an effort to remove these two drawbacks of the theory, Goudsmit and Uhlenbeck proposed in 1925 that an electron must be looked upon as a changed sphere spinning about its own axis, having an intrinsic (built-in) angular momentum and consequently an intrinsic magnetic dipole moment. These are called 'spin angular momentum' S and 'spin magnetic dipole moment' M, respectively.

Let us write the magnitude S of the spin angular momentum of the electron in terms of a 'spin quantum number’s, as we do for the orbital angular momentum L in terms of orbital quantum number l. Thus S

S=\sqrt{s(s+1)}\frac{h}{2\pi}
The only value which the spin quantum number can be given is s = ½, which confirms the observed fine-structures doubling.

S=\sqrt{\frac{1}{2}(\frac{1}{2}+1)}\frac{h}{2\pi}=\frac{\sqrt{3}}{2}\frac{h}{2\pi}

The component of S along a magnetic field parallel to the z-direction is

s_z=m_s\frac{h}{2\pi}

Where ms is the 'spin magnetic quantum number' and takes (2s + 1) = 2 values which are +s and -s, that is

ms= +1/2 and-1/2

The gyromagnetic ratio for electron spin μs/S is double the equivalent ratio μL/L=e/2m, according to experimental evidence.

The spinning electron was successful in describing not only fine structure and the strange Zeeman Effect, but also other atomic phenomena. Although electron spin was proposed as a postulate, Dirac established in 1928 that an electron must have an intrinsic rotational momentum and an intrinsic magnetic moment using relativistic quantum mechanics.

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Experimental evidence of electron spin:

• AH Compton proposed that “the electron is probably the ultimate magnetic particle” in Compton Scattering (1921).

• Stern-Gerlach Experiment (1922): A beam of silver atoms was passed through an inhomogeneous magnetic field, and two beams of space quantized components were seen.

• Uhlenbeck and Goudsmit (1925) demonstrated that there are two angular momentum states: intrinsic angular momentum of the electron and "SPIN" angular momentum.

• Pauli Exclusion Principle (1925): no more than two electrons per orbital, or no two electrons with identical quantum numbers. A new quantum number has been proposed.

Postulate 6: Under all conditions, all electronic wave functions must be ant symmetric.

graphical representation of angular and orbital angular momentum.

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Theoretical Justification:

Dirac (1928) developed relativistic quantum theory & derived electron spin angular momentum

  • Orbital Angular Momentum

L = orbital angular momentum

Formula of orbital angular momentum/Orbital angular momentum formula,

L=h\sqrt{l(l+1)}
l = orbital angular momentum quantum number

l\leq n-1
Lz = mℏ

m = 0, ±1, ±2… ±l

  • Spin Angular Momentum

S ≡ spin angular momentum

S=h\sqrt{s(s+1)}=h\frac{\sqrt{3}}{2}

s = spin angular momentum quantum number

s = ½

S = ms

m = ± 1/2

Angular Momentum of Electron in Hydrogen Atom:

De Broglie's hypothesis can be used to compute the angular momentum of the hydrogen atom of an electron.

Consider an electron moving in a circular orbit of radius r.

According to the Broglie hypothesis, the associated wavelength of any particle is:

\lambda =\frac{h}{M_v}....(1)

From classical mechanics, the orbital angular momentum formula is:

L = Mvr …. (2) Also known as mvr formula

It is also noted that

2πr = mλ

\lambda =\frac{2\pi r}{m}

By inserting the value of λ in equation (1), we get:

\frac{2\pi r}{m}=\frac{h}{M_v}...(3)

From equation 1 we can get:

M_v=\frac{L}{r}

By substituting the Mv in equation (3) we get:

\frac{2\pi r}{m}=\frac{h}{(\frac{l}{r})}=\frac{rh}{L}

Now, solve this relation for angular momentum L:

L=rh\times \frac{m}{2\pi r}

or, L=\frac{mh}{2\pi }

or, L=m.\frac{h}{2\pi}

Here, \frac{h}{2\pi} is designated ash.

So, the angular momentum of the electron of Hydrogen atom is:

L = m.ℏ

Here, m = 1, 2, 3, 4 …so on

Also, the angular momentum is quantized in units of ħ.

In hydrogen atom,

The radius of nth orbit is

rn n2 /Z

NCERT Physics Notes :

Where, Z is atomic number

So,

n=(zr_n)^\frac{1}{2}....(1)

Angular momentum of an electron in an orbit is given by,

L=\frac{nh}{2\pi}.....(2)

Put value of n from (1) in equation (2)

Angular momentum of electron in nth orbit, L=\frac{(zr_n)^{\frac{1}{2}}h}{2\pi}

L ∝ r1/2

L∝ √r

Hence, angular momentum of electron in hydrogen atom is proportional tor.

We can now tell the angular momentum in different orbits, say, angular momentum of electron in 5th orbit is 25h.

The following is a summary of everything we've learned so far about the energy and dispersion of an electron in a hydrogen atom:

  • The energy grows as n grows, and it is solely dependent on n, the fundamental quantum number.
  • As n grows, the average distance between the electron and the nucleus increases.
  • As n increases, the number of nodes in the probability distribution grows.
  • As l is increased, the electron density concentrates along certain lines (or in planes).

Bohr’s quantisation condition states: In Bohr’s model, the angular momentum of electrons orbiting around the nucleus is quantized on a condition that the electrons can move only in orbits with an integral multiple of h/2 angular momentum.

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Frequently Asked Questions (FAQs)

Q: How does the angular momentum of electrons contribute to the stability of certain electron configurations?
A:
Certain electron configurations, like those with completely filled or half-filled subshells, are particularly stable. This stability is partly due to the balanced arrangement of angular momenta in these configurations. For example, in a filled subshell, the orbital angular momenta of the electrons sum to zero, contributing to the overall stability of the atom or ion.
Q: What is the relationship between an electron's angular momentum and its magnetic quantum number?
A:
The magnetic quantum number (ml) specifies the projection of the electron's orbital angular momentum along a chosen axis (usually the z-axis in the presence of a magnetic field). It can take integer values from -l to +l, where l is the azimuthal quantum number. This quantization of angular momentum orientation is crucial in understanding atomic behavior in magnetic fields.
Q: How does the concept of angular momentum contribute to our understanding of the photoelectric effect?
A:
While the photoelectric effect is primarily explained by the particle nature of light, angular momentum plays a role in the details of the process. The conservation of angular momentum in the interaction between photons and electrons influences the directionality of electron emission and helps explain certain aspects of the photoelectric effect in materials with complex band structures.
Q: What is the significance of the Larmor precession in relation to electron angular momentum?
A:
Larmor precession describes the motion of the magnetic moment vector of an electron around an external magnetic field. This precession is directly related to the electron's angular momentum. The frequency of this precession (Larmor frequency) is proportional to the strength of the magnetic field and is important in phenomena like nuclear magnetic resonance.
Q: How does the angular momentum of electrons relate to the concept of electron configuration?
A:
Electron configuration describes how electrons are distributed in an atom's orbitals. The Aufbau principle, Hund's rule, and the Pauli exclusion principle govern this distribution, all of which are based on the angular momentum properties of electrons. The order of filling orbitals (1s, 2s, 2p, etc.) reflects increasing energy and angular momentum.
Q: Why is it important to consider both orbital and spin angular momentum when studying atomic spectra?
A:
Both orbital and spin angular momentum contribute to the total angular momentum of an electron, which determines the fine structure of atomic spectra. The interaction between orbital and spin angular momenta (spin-orbit coupling) leads to energy level splitting, resulting in more complex spectral patterns that provide detailed information about atomic structure.
Q: What is the significance of the total angular momentum quantum number in atomic physics?
A:
The total angular momentum quantum number (J) combines the orbital (L) and spin (S) angular momenta of an electron. It's crucial for understanding the fine structure of atomic spectra and the behavior of atoms in magnetic fields. The allowed values of J determine the possible energy states and transition rules in complex atoms.
Q: How does the angular momentum of electrons in multi-electron atoms differ from that in hydrogen?
A:
In multi-electron atoms, electron-electron interactions complicate the angular momentum picture. While the basic principles remain the same, the presence of other electrons leads to phenomena like orbital hybridization and electron correlation, which affect the overall angular momentum states of the atom.
Q: What is the connection between angular momentum and the fine structure in atomic spectra?
A:
Fine structure in atomic spectra arises from the interaction between an electron's orbital angular momentum and its spin angular momentum. This spin-orbit coupling leads to slight energy level splits, resulting in closely spaced spectral lines that reveal more detailed information about atomic structure.
Q: How does the uncertainty principle affect our ability to measure an electron's angular momentum?
A:
The uncertainty principle limits our ability to simultaneously measure an electron's position and momentum with arbitrary precision. This affects angular momentum measurements because angular momentum is related to both position (radius vector) and momentum. We can only determine probabilities for angular momentum values in certain states.