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Exercises · 2.56

Q.Calculate the wavelength for the emission transition if it starts from the orbit having radius 1.3225 nm and ends at 211.6 pm. Name the series to which this transition belongs and the region of the spectrum.

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The transition is from n=5n=5 to n=2n=2 in the hydrogen atom, giving a wavelength of 434.1 nm. This belongs to the Balmer series and lies in the visible region of the electromagnetic spectrum.

The key to solving this problem is recognising that the radii of Bohr orbits in hydrogen are quantised. Each orbit has a specific radius that depends only on the principal quantum number nn. Once we know the nn values for the initial and final orbits, we can use the Rydberg formula to find the wavelength of the emitted photon. The series and spectral region then follow directly from the nn values.

Let’s work through it step by step.

  1. Recall the Bohr radius formula. For a hydrogen-like atom (here, hydrogen itself, Z=1Z=1), the radius of the nn-th orbit is given by:

rn=n2a0r_n = n^2 a_0

where a0=52.9 pma_0 = 52.9\ \text{pm} (the Bohr radius). This is a fundamental result: the radius scales as n2n^2.

Watch out

A common mistake is to forget that the radius is proportional to n2n^2, not nn. Doubling nn quadruples the radius.

  1. Find the principal quantum number for the initial orbit. The initial radius is given as 1.3225 nm1.3225\ \text{nm}. Convert to picometres for consistency:

1.3225 nm=1322.5 pm1.3225\ \text{nm} = 1322.5\ \text{pm}

Using rn=n2a0r_n = n^2 a_0:

ni2=ria0=1322.5 pm52.9 pm=25n_i^2 = \frac{r_i}{a_0} = \frac{1322.5\ \text{pm}}{52.9\ \text{pm}} = 25

So ni=25=5n_i = \sqrt{25} = 5.

The electron starts in the n=5n=5 orbit.

  1. Find the principal quantum number for the final orbit. The final radius is 211.6 pm211.6\ \text{pm}. Again:

nf2=211.6 pm52.9 pm=4n_f^2 = \frac{211.6\ \text{pm}}{52.9\ \text{pm}} = 4

So nf=4=2n_f = \sqrt{4} = 2.

The electron ends in the n=2n=2 orbit.

  1. Use the Rydberg formula to calculate the wavelength. For a hydrogen atom, the wavenumber ν~\tilde{\nu} (inverse wavelength) for a transition from nin_i to nfn_f is:

1λ=RH(1nf2−1ni2)\frac{1}{\lambda} = R_H \left( \frac{1}{n_f^2} - \frac{1}{n_i^2} \right)

where RH=1.097×107 m−1R_H = 1.097 \times 10^7\ \text{m}^{-1} (the Rydberg constant).

Here ni=5n_i = 5, nf=2n_f = 2:

1λ=1.097×107(122−152)=1.097×107(14−125)\frac{1}{\lambda} = 1.097 \times 10^7 \left( \frac{1}{2^2} - \frac{1}{5^2} \right) = 1.097 \times 10^7 \left( \frac{1}{4} - \frac{1}{25} \right)

Compute the bracket: …

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