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By keeping the electrons in circular, quantized orbits around the positively-charged nucleus, Bohr was able to calculate the energy of an electron in the n th energy level of hydrogen: E ( n) = − 1 n 2 ⋅ 13.6 eV , where the lowest possible energy or ground state energy of a hydrogen electron— E ( 1) —is − 13.6 eV .
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