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Nuclear Rotations |
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Aage Bohr and Ben Mottleson found that nuclear rotations obey the I(I+1) rule; i.e., have energy levels E_{I} such that
where I is an integer, J is the moment of interia of the rotating nuclear shell and h is
Planck's constant divided by 2π. Note what this implies about the quantification of angular momentum.
If ω is the rate of rotation then
Thus angular momentum L is given by
This is in contrast to the Old Quantum Physics of Niels Bohr in
which L would be hI.
Note that
and thus the smaller the moment of inertia the faster a structure rotates.
However the angular momentum is always h²[I(I+1)]]^{½}.
Thus there is an equipartition of angular momenta among the various modes of rotation.
An alpha particle consists of two protons and two neutrons. Neutrons have slightly more mass than protons. For purposes of this order of magnitude estimate the differences between the neutron and the proton will be ignored. It is thus the computation for a pseudo-alpha particle.
The diameter of the alpha particle is approximately 3.6 fermi. The charge radius of a proton is 0.877 fermi. Deducting two proton radii from the diameter of the alpha particle gives a separation distance of the particle centers of 1.846 fermi and thus an orbit radius of 0.923 fermi.
The mass of an alpha particle is 6.64466×10^{-27} kg. Thus the moment of inertia of a alpha particle for rotation about an axis perpendicular to its longitudinal axis is
The minimum rate of rotation is thus
The number of complete rotations per second is 4.194×10^{21}.
Thus the order of magnitude of the rotations of a alpha particle is about 10^{20} per second.
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