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Thermal energies for nucleons in large nuclei are comparable with their binding energies of about 6 MeV.
(a) To what temperature does this correspond?
(b) Within nuclear matter, identical nucleons are separated by about 2.6 × 10-15 m. What is roughly the minimum temperature needed for them not to be degenerate (i.e., for the number of accessible states to be much larger than the number of particles.)?
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