The 656 nm line is the well‑known H‑α line in the Balmer series.
Common Pitfalls
Mixing up \$E1\$ and \$E2\$ – \$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.