According to Bohr, the quantization of the angular momentum of electrons is
On the other hand, we know that the angular momentum, according to quantum mechanics, is
Of course, as we see, the two equation are different:
However, we can say that "n\\approx\\sqrt{n^2-n}" for very large values of "n". This criterion leads to "L>>\\hbar". Therefore, according to the first equation ("L=mvr=n\\hbar"), we see that this is only possible for very large values of "r".
Hence, to describe the motion of an electron in terms of classical mechanics, we need "r>>a_0". As we saw above, this is only possible for very big "n", which leads to "L>>\\hbar".
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