Microwave/Rotational Spectroscopy

In summary, rotational (microwave) spectroscopy involves measuring the Kth energy level, which is equal to BK(K+1) with a constant B. The Kth energy level is found to be (2K+1) degenerate. This means that unmeasured molecules can occupy multiple states, but when measured, they are only found in one state. The number of molecules in each state follows a Boltzmann distribution, determined by degeneracy, at thermal equilibrium. However, this distribution does not directly relate to the likelihood of transitions between states. The spectral line intensities in rotational transitions depend on the number of molecules available to undergo the transition.
  • #1
Master J
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In rotational (microwave) spectroscopy, the Kth energy level is BK(K + 1), B = constant.

It turns out the each Kth level is (2K + 1) degenerate.

Now, as the energy level increases, does this mean that a single molecule will be in all these states at once, or in one of them? Or does it mean that the number of MOLECULES undergoing a transition to a higher energy state increases?

I am confused about the interpretation of this.

I know that the spectrum gives a nice curve shape, increasing first, because of ^^^^ and then decreasing because of the Boltzmann Population Law ( the no. of molecules undergoing transitions to higher states decreases as the energy between the states increases).

I hope someone can clarify what is actually going on here. Thanks!:smile:
 
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  • #2
Master J said:
Now, as the energy level increases, does this mean that a single molecule will be in all these states at once, or in one of them?

Quantum mechanically, an unmeasured molecule will occupy several states. But a single molecule can only ever be measured to be in a single state. Degeneracy doesn't enter into it.

When you measure an ensemble of molecules, you get a Boltzmann distribution of the populations of the states, that is the proportion of molecules in each state. Degeneracy does enter into that equation, directly.

On the other hand, the Boltzmann distribution say nothing at all about transitions. It just says which states a molecule is likely to be in, when at thermal equilibrium. Nothing about the likelihood of transitions, which isn't at all directly related to either the energy or degeneracy of the original or excited state. It's just that with rotational transitions, the transition-probability is more or less the same between every state, so then the spectral line intensities will depend entirely on the number of molecules available to do a transition, hence the Boltzmann-distributed shape.
 
  • #3


In rotational (microwave) spectroscopy, the Kth energy level is given by BK(K+1), where B is a constant. This means that as the energy level increases, the spacing between energy levels also increases. Each Kth level is also (2K+1) degenerate, which means that there are multiple energy states within each K level that have the same energy.

To answer your question, a single molecule can only occupy one energy state at a time. As the energy level increases, the molecule can only occupy one of the energy states within that level. However, there may be multiple molecules undergoing transitions to higher energy states at the same time, which is why we see a spectrum with multiple peaks.

The shape of the spectrum is determined by the number of molecules occupying each energy state, which follows the Boltzmann Population Law. As the energy difference between states increases, the number of molecules occupying the higher energy states decreases, resulting in a decrease in the intensity of the spectral lines.

In summary, the interpretation of this data is that a single molecule can only occupy one energy state at a time, but there may be multiple molecules undergoing transitions to higher energy states. The shape of the spectrum is determined by the number of molecules occupying each energy state, which is affected by the energy difference between states. I hope this clarifies things for you.
 

What is microwave/rotational spectroscopy?

Microwave/rotational spectroscopy is a type of spectroscopy that uses microwave radiation to study the rotational transitions of molecules. It provides information about the structure, chemical bonds, and other properties of molecules.

How does microwave/rotational spectroscopy work?

In microwave/rotational spectroscopy, a beam of microwaves is passed through a sample of molecules, causing the molecules to rotate. The amount of energy absorbed or emitted by the molecules during this rotation can be measured and used to identify the molecules and their properties.

What are the applications of microwave/rotational spectroscopy?

Microwave/rotational spectroscopy has many applications in various fields such as chemistry, physics, astronomy, and atmospheric science. It is used to identify and study the structure and properties of molecules, determine molecular concentrations, and analyze the composition of gases in the atmosphere.

What are the advantages of using microwave/rotational spectroscopy?

One of the main advantages of using microwave/rotational spectroscopy is that it is non-destructive, meaning the sample is not altered or destroyed during the analysis. It also has high sensitivity and can detect even small amounts of molecules in a sample. Additionally, it is a highly precise and accurate technique.

What are the limitations of microwave/rotational spectroscopy?

One limitation of microwave/rotational spectroscopy is that it can only be used to study molecules with a permanent dipole moment. This means that it is not suitable for studying symmetrical molecules such as homonuclear diatomic molecules. Additionally, the equipment required for this technique can be expensive and complex to operate.

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