Quantization Of Angular Momentum | Magnitude Quantization - Space quantization

Introduction:
Angular momentum plays a very important role in physics. It is a conserved quantity. Conserved quantities are those quantities that remain constant as the system evolves, unless some kind of an external force acts upon that system.
More explicitly we can say that - if there is a certain body that has a rotational motion with respect to an origin or an axis then there is a physical quantity known as angular momentum associated with it's rotation. It will remain constant until and unless some kind of an external torque acts upon that system.
Because of this very reason angular momentum plays a very important role not only in classical mechanics ( i.e. In classical systems where you might study how planets revolve around the sun in the solar system ) but also it plays a very important role in quantum mechanical systems ( like an electron revolving around the nucleus).
In the case of nuclear physics it is also quite important to study the spin and the angular momentum of the nucleus and the properties associated with that (like nuclear magnetic moment etc.).
To study the angular momentum of the nucleons and the electrons, first of all, we have to look into the orbital rotational momentum then the spin of these particles. In both these two cases, we have the quantization of both the magnitude and direction of these particular quantities. In this part we are going to study about it in detail.
Angular Momentum of a Classical system:
Before discussing quantum mechanical systems, let’s first look at a classical system. For example let us consider the solar system. Now, in the case of the Solar System, the Earth is revolving around the Sun. Besides the revolving, the earth rotates about its own axis.
Thus, the earth has two types of angular momenta - one is associated with the revolution of earth around the sun that is known as orbital angular momentum, and the other is associated with the rotation about earth’s own axis which is known as the spin angular momentum.
1. Orbital angular Momentum of a Classical system:
We may write the earth’s orbital angular momentum(L) as -
Where, = Position vector of earth from the axis of rotation.
and, represents the linear momentum of Earth’s orbital motion.
Thus, is perpendicular to both
and
i.e. it is perpendicular to the plane of the orbit.
Earth has a certain orbital velocity tangential to this particular orbit and that corresponds to the linear momentum . Angular or rotational momentum has a direction perpendicular to the plane in which the Earth moves around the Sun.
Angular momentum is a vector quantity. Then it has both magnitude and a particular direction. The magnitude tells us about the value of the angular momentum.
In the case of the solar system, the system itself does not put any restriction on the magnitude or the direction of the angular momentum. This means, if the earth suddenly starts spinning at a higher velocity then the magnitude of the angular momentum of Earth will increase.
Thus, angular momentum of Earth can take any value, depending upon the distance from the axis of rotation and the orbital velocity of Earth here. Therefore, the magnitude of angular momentum of earth can take a continuous range of values. A given planet can revolve in any elliptical plane and it can have any direction of angular momentum pointing in any direction in the three-dimensional space. This also means that angular momentum of Earth is not quantized.
Thus, the orbital angular momentum of classical systems are not quantized. That means they do not take discrete values. They can take any value depending upon the position vector of the rotating object with respect to the axis of rotation.
2. Spin angular Momentum of a Classical system:
The earth as a body itself is spinning on its own axis passing through its center. Then we have a spin motion of earth here. In that case also, we will have the magnitude of the spin angular momenta and the direction.
Spin angular momentum is also not quantized for all classical systems.
Quantization of Angular Momentum in Quantum-mechanical Systems:
Whenever we look into the quantum mechanical systems, the angular momentum can not take any magnitude or direction. It can take some discrete values only.
Let us take a simple example of an electron revolving around the nucleus. In this case we can see that the electron is not allowed to take any magnitude or direction of angular momentum. It can take some particular values only i.e. it is quantized here. We are going to discuss this phenomenon in detail in the next section.
The solution of the Schrodinger’s equation for the case of an electron in an atom results in certain quantum numbers and these quantum numbers put restrictions on the magnitude and the direction of the angular momentum of the electron.
Orbital angular Momentum of a Quantum-Mechanical System:
Let’s, first look at the orbital angular momentum of electron in hydrogen atom.1. Quantization of Magnitude:



Thus , L can not take a continuous range of values; it can only take certain discrete values which is allowed by this particular equation given above. This is known as the quantization of the magnitude of the angular momentum.
For example, let's look at the S orbital. In the case of S orbital , we have azimuthal quantum number l=0. In that case the magnitude of the angular momentum would be equal to -


Similarly, for d orbital :

Thus, the magnitude of the angular momentum of the electron can only possess certain discrete values. Given by L=

2. Direction quantization or space quantization for Orbital Electron:

gives the z-component of the angular momentum of that particular orbit. This restriction is known as Direction quantization or space quantization .


For example, let us take the p orbital. In the case of a p orbital the azimuthal quantum number(l) has a value of 1. Then magnetic quantum number() can have the values -1,0,+1 .
Then, for the case of p orbital z component of orbital angular momentum() can have only three values,

We know that the electron's motion is confined in three dimensional space. Here , is the z component of orbital angular momentum.
If there is an external magnetic field present then we take the standard z-axis along the field direction. The electron is a charged particle moving in an orbit so it has a particular magnetic moment. So it will orient itself in such a direction that the z component of its angular momentum can take only the three values, as mentioned above.
Now, for example let us take =1. In this case angular momentum of the orbit can precess in such a direction that the z component of it can take only the value
.

In terms of 3D visualization the component can have a certain fixed value for a particular conical section. So there are three different conical sections which put a restriction on the direction of the angular momentum of the electron orbit.
Quantization of Spin Angular Momentum:
1. Quantization of Magnitude:


2. Quantization of direction:



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Thank you for your kind information.
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