Orthohydrogen to Parahydrogen: What particle?

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SUMMARY

The transition of diatomic Hydrogen (H2) from Orthohydrogen to Parahydrogen involves the emission of a photon. Cooling a sample of Hydrogen allows for the conversion of all H2 molecules to para- due to the dominance of lower energy states at low temperatures. In contrast, heating cannot exceed a 3:1 ratio of ortho- to para- because, at infinite temperature, the distribution of spin states remains fixed at this proportion, with three spin states for ortho and one for para. Thus, the equilibrium favors para hydrogen at absolute zero.

PREREQUISITES
  • Understanding of quantum mechanics and spin states
  • Familiarity with thermodynamic principles
  • Knowledge of photon emission and absorption processes
  • Basic concepts of molecular hydrogen behavior
NEXT STEPS
  • Research the principles of quantum spin and its implications in molecular hydrogen
  • Explore the thermodynamic behavior of gases at varying temperatures
  • Study photon interactions with matter, specifically in cooling processes
  • Investigate the implications of ortho- and para- hydrogen in chemical reactions
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Physicists, chemists, and students studying molecular behavior, thermodynamics, and quantum mechanics, particularly those interested in the properties of hydrogen and its applications in various scientific fields.

Chalmers
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What subatomic particle is emitted when a diatomic Hydrogen molecule transitions from Orthohydrogen to Parahydrogen? e.g. during cooling

And why can you cool a sample of Hydrogen to assure that all H2 molecules are para-, but you cannot heat to have any more than 3:1 ortho-:para- ?
 
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Chalmers said:
What subatomic particle is emitted when a diatomic Hydrogen molecule transitions from Orthohydrogen to Parahydrogen? e.g. during cooling

I assume a photon.

Chalmers said:
And why can you cool a sample of Hydrogen to assure that all H2 molecules are para-, but you cannot heat to have any more than 3:1 ortho-:para- ?

Well, what's the difference between ortho- and para-?
 
Chalmers said:
And why can you cool a sample of Hydrogen to assure that all H2 molecules are para-, but you cannot heat to have any more than 3:1 ortho-:para- ?

The short reason is that in the limit of infinite temperature, any given hydrogen molecule is equally likely to be in anyone of its four spin spin states. Since there are three spin states for ortho hydrogen and only one for para hydrogen, you get a fixed proportion of 3:1 even in the limit of infinite temperature.

At lower than infinite temperatures, lower energy states will be more likely to be occupied. Still, since there are three times as many high energy spin states to low energy spin states, you can have equilibrium proportions near 3:1 even at room temperature.

At very low temperatures (relatively speaking), the lower energy state is so much more likely to be occupied than any higher energy state, that the proportion goes down and down, until at absolute zero, you get a proportion of 0:1, with all the hydrogen being para hydrogen.
 

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