A particle of mass moves in circular orbits with potential energy

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Problem

A particle of mass mm moves in circular orbits with potential energy V(r)=FrV(r) = Fr, where FF is a positive constant and rr is its distance from the origin. Its energies are calculated using the Bohr model. If the radius of the particle's orbit is denoted by RR and its speed and energy are denoted by vv and EE, respectively, then for the nthn^{\text{th}} orbit (here hh is the Planck's constant) (1) R∝n1/3R \propto n^{1/3} and v∝n2/3v \propto n^{2/3} (2) R∝n2/3R \propto n^{2/3} and v∝n1/3v \propto n^{1/3} (3) E=32(n2ℏ2F24π2m)1/3E = \frac{3}{2} \left( \frac{n^2 \hbar^2 F^2}{4\pi^2 m} \right)^{1/3} (4) E=2(n2ℏ2F24π2m)1/3E = 2 \left( \frac{n^2 \hbar^2 F^2}{4\pi^2 m} \right)^{1/3}

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