Each
hydrogen molecule (H2) consists of two
hydrogen
atoms linked by a
covalent
bond. If we neglect the traces of
deuterium and
tritium which could be present,
each
hydrogen
atom consists of one
proton and one
electron. The proton has an
associated
magnetic
moment, which we can treat as being generated by the proton's
spin. The spins of the two hydrogen atoms can either be aligned the
same direction (this is orthohydrogen) or in opposite directions
(this is parahydrogen). The ratio between the ortho and para forms
is about 3:1 at
standard temperature and pressure, but the para form dominates
at low temperatures (approx. 99.95% at 20 K). Other molecules and
functional groups containing two hydrogen atoms, such as
water
and
methylene, also
have ortho and para forms, although their ratios differ from that
of the dihydrogen molecule.
Orthohydrogen is unstable at low temperatures and
spontaneously changes into parahydrogen, but the process is slow
because the kinetic barrier to interconversion is high. The
conversion from ortho to para state is
exothermic (releasing heat).
The presence of a paramagnetic substance in liquid hydrogen can
induce rapid heating - an undesirable occurrence when one wants
hydrogen to remain liquid. At room temperature, hydrogen contains
75% orthohydrogen, a proportion which the liquefaction process
preserves. One must therefore use a
catalyst to accelerate the
conversion of the liquid hydrogen into parahydrogen, or supply
additional refrigeration equipment to absorb the heat that the
liquid hydrogen will give off as it spontaneously converts itself
to pure parahydrogen.
The first synthesis of pure parahydrogen was
achieved by
Paul Harteck
and
Karl
Friedrich Bonhoeffer in 1929.
References
orthohydrogen in French:
Orthohydrogène