If
then is large and the wall correction is exponentially small:
This is exactly the equipartition theorem result from the two kinetic and two harmonic-potential quadratic terms.
If , use
Then
The leading term is the kinetic energy. The particle is nearly uniform in the disk, so and , much smaller than . The hard wall therefore suppresses the positional equipartition contribution, as in the hard-wall correction to harmonic equipartition.

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