The Balmer series is a set of spectral lines of hydrogen that appear when electrons transition from higher energy levels down to the second energy level, or n=2. These transitions result in the emission of light in the visible spectrum, which is why they are often colorful.
However, not every emission line resulting from electron transitions belongs to the Balmer series. Only those where the electron ends at the second energy level do. The formula used to determine the wavelength of light emitted in the Balmer series is:
- \( \frac{1}{\lambda} = R_H \left( \frac{1}{2^2} - \frac{1}{n^2} \right) \)
where \( \lambda \) is the wavelength, \( R_H \) is the Rydberg constant \( (1.097373 \times 10^7 \, \text{m}^{-1}) \), and \( n \) is an integer greater than 2. If the derived \( n \) is a whole number and greater than 2, the wavelength belongs to the Balmer series.