Explain the amount of light absorbed by a solution of molecules or ions in relationship to the concentration, path length, and molar absorptivity.
The Beer–Lambert law relates the light absorbed by a solution to three variables:
A = εbc
In most experiments path length and wavelength are held constant, so absorbance is directly proportional to concentration. That turns the law into a practical measuring tool: prepare standards of known concentration, plot A versus c, and read an unknown off the resulting straight calibration line. The slope is εb.
EK 3.13.A.2 also specifies the experimental design point: the spectrophotometer is set to the wavelength of maximum absorbance (λ_max) for the species being analyzed, to ensure maximum sensitivity of measurement. At λ_max a small change in concentration produces the largest change in absorbance.
Sources of error — this topic's science practice is about identifying them: a fingerprinted or scratched cuvette, failing to blank the instrument with pure solvent, bubbles in the light path, a colored impurity that absorbs at the same wavelength, or working outside the linear range at very high absorbance.
A student prepares standards of a blue dye and measures absorbance at λ_max in a 1.00 cm cuvette: 0.0200 M → A = 0.410; 0.0400 M → A = 0.815; 0.0600 M → A = 1.220. An unknown gives A = 0.590. Find the molar absorptivity and the unknown concentration.
Molar absorptivity. The data are linear, so use the slope:
slope = (1.220 − 0.410)/(0.0600 − 0.0200) = 0.810/0.0400 = 20.25 M⁻¹
Since slope = εb and b = 1.00 cm,
ε = 20.3 M⁻¹cm⁻¹
Unknown concentration.
c = A/(εb) = 0.590 ÷ (20.25 × 1.00) = 0.0291 M
Check: 0.590 lies between the 0.410 and 0.815 standards, so the concentration should lie between 0.0200 and 0.0400 M ✓ — and the answer is safely inside the calibrated range.