Answer:
According to Bohr's theory, only such orbits are permissible for the motion of an electron around the nucleus in which the angular momentum of an electron is integral multiple of \[h/2\pi \]. \[L=m\upsilon r=\frac{nh}{2\pi },\] \[n=1,2,3,....\] Here \[\mathbf{n}\] is the principal quantum number.
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