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Exercises · 2.13

Q.What is the wavelength of light emitted when the electron in a hydrogen atom undergoes transition from an energy level with n = 4 to an energy level with n = 2?

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The wavelength of light emitted when an electron in a hydrogen atom drops from n=4n=4 to n=2n=2 is found using the Rydberg formula. The result is 486 nm (blue-green light).

The key to this problem is understanding energy level quantization in the hydrogen atom. Niels Bohr proposed that electrons can only occupy specific, discrete energy levels, labelled by the principal quantum number nn. When an electron jumps from a higher energy level (n=4n=4) to a lower one (n=2n=2), it loses energy. That energy isn't destroyed — it is emitted as a single photon of light. The photon's energy is exactly equal to the difference between the two energy levels.

The wavelength of that photon is then given by the Planck-Einstein relation: E=hcλE = \frac{hc}{\lambda}, where hh is Planck's constant, cc is the speed of light, and λ\lambda is the wavelength. So, the problem reduces to calculating the energy difference ΔE=E4−E2\Delta E = E_4 - E_2, and then converting that to a wavelength.

The energy of an electron in the nn-th level of a hydrogen atom is given by:

En=−13.6 eVn2E_n = -\frac{13.6 \text{ eV}}{n^2}

This negative sign means the electron is bound to the nucleus; the more negative the energy, the more stable (lower) the level.

Let's work through the calculation step by step.

  1. Find the energy of the n=4n=4 level.

E4=−13.642=−13.616=−0.85 eVE_4 = -\frac{13.6}{4^2} = -\frac{13.6}{16} = -0.85 \text{ eV}

  1. Find the energy of the n=2n=2 level.

E2=−13.622=−13.64=−3.40 eVE_2 = -\frac{13.6}{2^2} = -\frac{13.6}{4} = -3.40 \text{ eV}

  1. Calculate the energy difference ΔE\Delta E (the energy of the emitted photon). The photon's energy is the energy lost by the atom, so:

ΔE=E4−E2=(−0.85)−(−3.40)=+2.55 eV\Delta E = E_4 - E_2 = (-0.85) - (-3.40) = +2.55 \text{ eV}

The positive sign indicates energy is released.

Tip

A faster way to get ΔE\Delta E directly is to use the formula:

ΔE=13.6(1nf2−1ni2) eV\Delta E = 13.6 \left( \frac{1}{n_f^2} - \frac{1}{n_i^2} \right) \text{ eV}

where nin_i is the initial level (4) and nfn_f is the final level (2). This gives the same result: 13.6(14−116)=13.6×316=2.55 eV13.6 \left( \frac{1}{4} - \frac{1}{16} \right) = 13.6 \times \frac{3}{16} = 2.55 \text{ eV}.

  1. Convert the energy from eV to Joules. The Planck-Einstein relation uses SI units. Since 1 eV=1.602×10−19 J1 \text{ eV} = 1.602 \times 10^{-19} \text{ J}:

ΔE=2.55 eV×1.602×10−19 J/eV=4.085×10−19 J\Delta E = 2.55 \text{ eV} \times 1.602 \times 10^{-19} \text{ J/eV} = 4.085 \times 10^{-19} \text{ J}

  1. Use the Planck-Einstein relation to find the wavelength. The relation is E=hcλE = \frac{hc}{\lambda}, so λ=hcE\lambda = \frac{hc}{E}. Using h=6.626×10−34 J sh = 6.626 \times 10^{-34} \text{ J s} and c=3.00×108 m/sc = 3.00 \times 10^8 \text{ m/s}: …

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