According to Bohr's model of the hydrogen atom,
(A) the radius of the orbit of an electron is directly proportional to n.
(B) the speed of the orbiting electron is directly proportional to 1/n
(C) the total energy of the electron is directly proportional to 1/n2
(D) the radius of the orbit of an electron is directly proportional to n2
Choose the correct answer from the options given below:
Answer & explanation
Correct answer: option 2
The correct answer is Option (2) → (B), (C) and (D) only
In the Bohr model, the electron moves in a circle under the Coulomb attraction of the nucleus, and only those orbits are allowed in which the angular momentum is quantised, \( mvr = nh/2\pi \). Solving these two conditions together gives, for hydrogen:
\( \displaystyle r_n = \frac{\varepsilon_0 n^{2} h^{2}}{\pi m e^{2}} = 0.53\,n^{2}\,\text{angstrom} \Rightarrow r_n \propto n^{2} \)
\( \displaystyle v_n = \frac{e^{2}}{2\varepsilon_0 n h} \Rightarrow v_n \propto \frac{1}{n} \)
\( \displaystyle E_n = -\frac{m e^{4}}{8\varepsilon_0^{2} n^{2} h^{2}} = -\frac{13.6}{n^{2}}\,\mathrm{eV} \Rightarrow E_n \propto \frac{1}{n^{2}} \)
(A) the radius of the orbit of an electron is directly proportional to n. — Incorrect. The radius is proportional to n2, not to n: the second orbit is four times as large as the first.
(B) the speed of the orbiting electron is directly proportional to 1/n — Correct. The speed is greatest in the first orbit (about 2.2 × 106 m s−1) and falls as 1/n in the outer orbits.
(C) the total energy of the electron is directly proportional to 1/n2 — Correct. \( E_n = -13.6/n^{2} \) eV; the constant of proportionality is negative because the electron is bound, so the energy rises towards zero as n increases.
(D) the radius of the orbit of an electron is directly proportional to n2 — Correct. This follows from \( r_n = 0.53\,n^{2} \) angstrom worked out above.
NCERT (2026-27):
Bohr Model of the Hydrogen Atom – “… Eq. (12.14) depicts that the orbital speed in the \( n^{\mathrm{th}} \) orbit falls by a factor of \( n \). … From Eq. (12.15), it can also be seen that the radii of the orbits increase as \( n^{2} \). The total energy of the electron in the stationary states of the hydrogen atom can be obtained by substituting the value of orbital radius in Eq. (12.4) as
\( \displaystyle E_n = -\left(\frac{e^{2}}{8\pi\varepsilon_0}\right)\left(\frac{m}{n^{2}}\right)\left(\frac{2\pi}{h}\right)^{2}\left(\frac{e^{2}}{4\pi\varepsilon_0}\right) \)
or
\( \displaystyle E_n = -\frac{m e^{4}}{8 n^{2}\varepsilon_0^{2} h^{2}} \qquad (12.17) \)”