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Here we deduce nuclear vibrations from the harmonic oscillator and nuclear rotations from the total energy of the rigid rotor, which assumes that the distance between particles remain the same (i.e. V=0). Hence, we quantize the classical kinetic energy and obtain the eigenvalues for the rigid rotor. In nuclear physics, this is called the rotational flow model to avoid the implication that nucleons are frozen in position. Although this is an idealization, the excitation energies nicely match the predicted J(J+1) pattern, which characterizes the excitation of deformed nuclei in the mass 180 region and the rare earth.