A particle of mass m moves in a circular orbit in a central potential field U(r) = 1/2kr². If Bohr's quantization condition is applied, radii of possible orbitals and energy levels vary with quantum number n as:
rₙ∝√n, Eₙ∝1/n
rₙ∝√n, Eₙ∝n
rₙ∝n², Eₙ∝1/n²
rₙ∝n, Eₙ∝n
Solution:
The correct option is D rₙ∝√n, Eₙ∝n F = dV/dR = kr = mv²/r mvr = nħ/2π r²∝n r∝√n E = 1/2kr² + 1/2mv²∝r²∝n