Concept:
- Microwave Spectroscopy: Involves the study of the rotational transitions of gas-phase molecules, providing information on molecular structure and bond lengths.
- Rotational Constant (B): Given by the formula B=8π2Ich , where h is Planck's constant, I is the moment of inertia, and c is the speed of light.
- Moment of Inertia (I): For a diatomic molecule, I=μr2, where μ is the reduced mass and r is the bond length.
- Energy Levels and Transitions: The energy associated with rotational levels is given by EJ = B J (J + 1) , and the positions of spectral lines are determined by transitions such as ΔJ=±1 .
Explanation:
To calculate the position of the second line in the microwave spectrum, we need to determine the rotational constant B and use it to find the frequency of the second transition ( J=0→J=1 and J=1→J=2 ).
Moment of inertia ( I ):
I=μr2 where μ=mC+mNmC⋅mN and r=0.129×10−9 meters.
Approximate masses are:
mC = 12 u and mN = 14 u , where u is the atomic mass unit.
Using atomic mass unit u≈1.66×10−27 kg:
mC≈12×1.66×10−27,kg=1.992×10−26,kg
mN≈14×1.66×10−27,kg=2.324×10−26,kg
μ≈1.992×10−26+2.324×10−261.992×10−26×2.324×10−26=1.108×10−26,kg (approx).
Moment of inertia ( I ):
I=μr2=1.108×10−26×(0.129×10−9)2=1.842×10−46,kg⋅m2.
Rotational constant ( B ):
B=8π2Ich
Where h≈6.63×10−34,J⋅s and c≈3×1010,cm/s
B=8π2×1.842×10−46×3×10106.63×10−34 .
Therefore B :
B=8×9.87×1.842×10−46×3×10106.63×10−34( \approx \frac{6.63 \times 10^{-34}}{1.382 \times 10^{-34}}\) ≈4.80×1010,Hz .
Converting B to wavenumbers ( cm-1 ):
B=3×10104.80×1010≈1.60,cm−1 .
The position of the second line ( J = 1 → J = 2 ) will be 4B :
Position of second line=4×1.60=6.40,cm−1
Conclusion:
The position of the second line in the microwave spectrum is 6.264 cm-1.