Calculate the energy difference:
$$\Delta E = E_2 - E_3 = (-3.40) - (-1.51) = -1.89\ \text{eV}$$
Since the electron drops to a lower level, the photon energy is $|\Delta E| = 1.89\ \text{eV}$.
Convert to joules: $1\ \text{eV} = 1.602\times10^{-19}\ \text{J}$,
$$\Delta E = 1.89 \times 1.602\times10^{-19}\ \text{J} = 3.03\times10^{-19}\ \text{J}$$
The 656 nm line is the well‑known H‑α line in the Balmer series.
Common Pitfalls
Mixing up $E_1$ and $E_2$ – $E_1$ must be the higher (initial) energy for emission.
For absorption, the photon energy is still $hf = E_{\text{higher}} - E_{\text{lower}}$, but the electron moves upward.
Remember to convert electron‑volts to joules before using $h$.
Use $c = 2.998\times10^{8}\ \text{m s}^{-1}$ for accurate wavelength values.
Practice Questions
Calculate the wavelength of the photon emitted when an electron in a hydrogen atom falls from $n = 5$ to $n = 2$.
What is the frequency of the photon required to excite an electron from $n = 1$ to $n = 3$ in hydrogen?
Explain why the Balmer series appears in the visible region while the Lyman series is ultraviolet.
Suggested diagram: Energy level diagram for hydrogen showing the $n=1$ to $n=5$ levels and the transitions that give rise to the Lyman, Balmer and Paschen series.
Summary
• Atoms possess quantised energy levels.
• Transitions between levels produce photons whose energy is given by $hf = E_{\text{initial}} - E_{\text{final}}$.
• Using $c = \lambda f$, the wavelength of the emitted or absorbed light can be calculated.
• Mastery of this relationship allows prediction and interpretation of line spectra, a cornerstone of atomic physics.