Wednesday, January 30, 2019

Quantum numbers

Quantum numbers

The simplest definition of Quantum mechanics is that quantum mechanics is the part of science that explain the distribution of the electrons around the nucleus and calculate the energy of electrons.

There are four quantum numbers used to describe the distribution of the electrons in any atom. These numbers are derived from the mathematical solution of the Schrödinger equation for the hydrogen atom. The four quantum numbers are called:
a- The principal quantum number
b. The angular momentum quantum number
c. The magnetic quantum number
d. The spin quantum number
The first three are used to describe atomic orbitals and to label electrons that reside in them. The fourth quantum number describes the behavior of a specific electron and completes the description of electrons in atoms.

a. The Principal Quantum Number (n)
The principal quantum number (n) have to be an integer number (1, 2, 3,…….). For hydrogen atom only, the value of n determines the energy of an orbital. The principle quantum number can give information about the average distance of the electron from the nucleus is a particular orbital. The larger n is, the greater the average distance of an electron in the orbital from the nucleus and therefore the larger the orbital.

The Angular Momentum Quantum Number (l)
The angular momentum quantum number (l) give information about the “shape” of the orbitals. From the value of “n” we can determine the number of ‘l” value. For a given value of n, l has possible integral values from 0 to ( n -1). For example, If n = 1, there is only one possible value of l; ( l = n - 1 = 1 - 1 = 0). Another example, if n = 2, there are two values of l (l = 0 and 1). If n = 3, there are three values of l (l= 0, 1, and 2). The value of l is generally designated by the letters s , p , d , f, and so on.

l
0
1
2
3
4
5
Name of orbital
s
p
d
f
g
h

If n=1, l= 0 we have s orbital
If n=2, l=0 and 1 we have s and p orbitals
If n=3, l=0, 1 and 2 we have s, p and d orbitals and so on……………
( “s” stand for the spectral lines of atomic emission spectra, “p” stand for the strong emission of principal lines, “d” for the diffuse of the atomic emission spectra, and “f” for fundamental atomic spectra emission). After letter “f” the naming of orbital followed alphabetical order.
A collection of orbitals “l” with the same value of “nis frequently called a shell. If one or more orbitals with the same “nand “l values are referred to as a subshell. For example, the shell with n= 2 is composed of two subshells, l= 0 and 1 (the allowed values for n= 2). These subshells are called the 2s and 2p subshells where 2 denotes the value of n , and s and p denote the values of l.

The principle quantum no.
The Angular Momentum Quantum Number (l)
Orbital
Subshell
n=1
l=0
s orbital
1s
n=2
l= 0 and 1
s and p orbitals
1s, 2s, 2p

The Magnetic Quantum Number (ml)
The magnetic quantum number (ml) describes the orientation of the orbital in space. Within a subshell, the value of ml depends on the value of the angular momentum quantum number, l.
For a certain value of l, there are (2l+1) integral values of ml as follows:
- l, (-l+1),       0,           (+l-1), + l
Example: for l=0 ml=0
If l =1 then no. of ml= (1X2)+1=3  ml will have three values= -1, 0, 1
If l=2, then no. of ml = (2X2)+1 = 5 values, ml = -2, -1, 0 ,1, 2.
The number of ml values indicates the number of orbitals in a subshell with a particular l value.

The Electron Spin Quantum Number (ms )
The electromagnetic theory postulated that, a spinning charge generates a magnetic field, and it is this motion that causes an electron to behave like a magnet. The two possible spinning motions of an electron, one clockwise and the other counter clockwise.
The fourth quantum number, called the electron spin quantum number (ms ), which has a value of +½ , -½
Otto Stern and Walther Gerlach in 1924 experiment showed that the interaction between an electron and the magnetic field causes the atom to be deflected from its straight-line path. Because the spinning motion is completely random, the electrons in half of the atoms will be spinning in one direction, and those atoms will be deflected in one way; the electrons in the other half of the atoms will be spinning in the opposite direction, and those atoms will be deflected in the other direction. Thus, two spots of equal intensity are observed on the detecting screen.

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