Energy eigen value of Rigid rotator

In many cases the molecular rotation spectra of molecules can be described successfully with the assumption that they rotate as rigid rotors. In these cases the energies can be modeled in a manner parallel to the classical description of the rotational kinetic energy of a rigid object. From these descriptions, structural information can be obtained (bond lengths and angles). The most straightforward examples are those of diatomic molecules. Energy calculations in quantum mechanics involve the solution of the Schrodinger equation with a properly formulated Hamiltonian to represent the energy operator. The form of the Hamiltonian can often be implied from the nature of the classical energy of such a physical system. The process involves finding the quantum mechanical operators associated with the constituents of the system energy. The energy of a freely rotating rigid rotor is simply the rotational kinetic energy, which can be expressed in terms of the angular momentum.

Summary

In many cases the molecular rotation spectra of molecules can be described successfully with the assumption that they rotate as rigid rotors. In these cases the energies can be modeled in a manner parallel to the classical description of the rotational kinetic energy of a rigid object. From these descriptions, structural information can be obtained (bond lengths and angles). The most straightforward examples are those of diatomic molecules. Energy calculations in quantum mechanics involve the solution of the Schrodinger equation with a properly formulated Hamiltonian to represent the energy operator. The form of the Hamiltonian can often be implied from the nature of the classical energy of such a physical system. The process involves finding the quantum mechanical operators associated with the constituents of the system energy. The energy of a freely rotating rigid rotor is simply the rotational kinetic energy, which can be expressed in terms of the angular momentum.

Things to Remember

  1. . Energy eigen values of rigid rotator is discrete and energy is quantised.
  2. Each energy level is (2l+1) fold degenerate. [ i.e. there are (2l+1) wave function for each value of l and \(E_l\))
  3. The different wave function for each value of l and indicated by different values of m. For example For, l=3. there are 7 wave function having same energy \(E_3= 12 Bh\). 
  4. The separation between successive energy level increases linearly with quantum number l.
  5. The energy gap between successive level is not equal. ( Gap increases as we move towards higher energy level).
  6. The probability density corresponding to \(\psi_1^m(\theta, \phi)\) is always independent of \(\phi\). [ \(\phi\)= azimuthal angle]

    i.e Probability distribution is always symmetrical about z-axis as,

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Energy eigen value of Rigid rotator

Energy eigen value of Rigid rotator

Energy Eigen Value of Rigid rotator:

From equation (16) and (21)

$$\beta=\frac{2IE}{\hbar^2}=l(l+1)$$

$$\therefore\; E= \frac{\hbar l(l+1)}{2I}\dotsm(27)$$

It gives the energy eigen values of rigid rotator.

Equation (27) can be written in the form,

$$E_l= Bh l(l+1)\dotsm(28)$$

Where, \(B=\frac{h}{8\pi^2 I} \) ( Rotational constant )

$$B= \frac{h}{8\pi^2\mu r^2}$$

The value of l is given by l=0,1,2,3,...

$$E_0= 0$$

$$l=1, \; E_1= 2Bh$$

$$l=2,\; E_2= 68Bh$$

$$l=3,\; E_3 = 12 Bh$$

$$l=4,\; E_4= 20Bh$$

$$l=5,\; E_5= 30Bh$$ and so on.

1. Energy eigen values of rigid rotator is discrete and energy is quantised.

2. Each energy level is (2l+1) fold degenerate. [ i.e. there are (2l+1) wave function for each value of l and \(E_l\))

3. The different wave function for each value of l and indicated by different values of m. For example For, l=3. there are 7 wave function having same energy \(E_3= 12 Bh\). They are symbolised as,

$$\psi_l^m (\theta, \phi); [\psi_3^{-3}, \psi_3^{-2}, \psi_3^{-1}, \psi_3^{0}, \psi_3^1,\psi_3^2, \psi_3^3]$$

4. The separation between successive energy level increases linearly with quantum number l.

$$i.e \; E_{l+1}-E_l= Bh[ (l+1)((l+2)-l(l+1)]$$

$$=Bh(l^2+ 3l+ 2-l^2-1)$$

$$=2Bh(l+1)$$

$$\Rightarrow (E_{l+1}-E_l)\propto l+1$$

$$\Rightarrow (E_l-E_{l-1})\propto l$$

5. The energy gap between successive level is not equal. ( Gap increases as we move towards higher energy level).

6. The probability density corresponding to \(\psi_1^m(\theta, \phi)\) is always independent of \(\phi\). [ \(\phi\)= azimuthal angle]

i.e Probability distribution is always symmetrical about z-axis as,

$$\phi(\theta,\phi)= [\psi_l^m (\theta, \phi)]^*[\psi_l^m (\theta, \phi)]$$

$$=\biggl[\frac{2l+1}{4\pi}\frac{(l-m)!}{(l+m)!}\biggr] |P_l^m (cos\theta)^2| e^{-im\phi}\cdot e^{im\phi}$$

$$=\biggl[\frac{(2l+1)}{4\pi}\frac{(l-m)!}{(l+m)!}\biggr]|P_l^m (cos\theta)|^2= independent \; of \phi$$

$$= Symmetric \; about \; z-axis.$$

Fig:
Fig:

7. The energy level diagram of rigid rotator is given by;

Fig:
Fig:

Question : If Bound length of Hcl molecule is \(1.3 \; A^0\). Then determine the 1st four rotational energy levels of the molecules in terms of electron volt (ev).

\(\Rightarrow\) Soltuion:

Bond length of Hcl molecule (r) = \( 1.3^\circ= 1.3\times 10^{-10}m\)

mass of H-atom \( ( m_H)= 1\;amu\)

mass of chlorine atom \((m_{cl})= 35.5\; amu\)

$$\mu_{Hcl}= \frac{m_H\cdot m_{cl}}{m_H+ m_{cl}}$$

$$=\frac{1\times 35.5}{1+ 35.5}$$

$$=\frac{35.5}{36.5}$$

$$=0.97\; amu$$

$$=0.97\times 1.67\times 10^{-27}kg$$

Now,

$$B=\frac{h}{8\pi^2\mu_{Hcl}r^2}$$

$$=\frac{6.62\times 10^{-34}}{8\times (3.14)^2\times 0.97\times 1.67\times 10^{-27}\times (1.3\times 10^{-10})^2}$$

$$=3.06\times 10^{11}sec^{-1}$$

Now, Rotational energy of Hcl molecule is,

$$E_l= Bh(l+1)\; For l= 0,1,2,3,..$$

$$For\; l=0, E_0=0$$

$$For \; l=1, E_1= 2Bh= 2\times 3.06\times 10^{11}\times 6.62\times 10^{-34}$$

$$=4.05\times 10^{-22}J$$

$$=\frac{4.05\times 10^{-22}}{1.602\times 10^{-19}}ev$$

$$=2.62\times 10^{-34}ev$$

$$For\; l=2, E_2= 6Bh=6\times 3.06\times 10^{11}\times 6.62\times 10^{-34}$$

$$=7.58\times 10^{-3}ev$$

$$For,\;l=3, E_3= 12Bh= 12\times 3.06\times 10^{11}\times 6.62\times 10^{-34}$$

$$=0.015ev$$

Reference:

  1. Mathews, P.M and K Venkatesan.A Text Book of Quantum Mechanics.New Delhi: Tata McGraw Hill Publishing Co. Ltd, 1997.
  2. Merzbacher, E.Quantum Mechanics .New York: John Wiley, 1969.
  3. Prakash, S and S Salauja.Quantum Mechanics.Kedar Nath Ram Nath Publishing Co, 2002.
  4. Singh, S.P, M.K and K Singh.Quantum Mechanics.Chand & Company Ltd., 2002.

Lesson

Harmonic oscillator and Application

Subject

Physics

Grade

Bachelor of Science

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