Syllabus topics (RTMNU)
- Electromagnetic spectrum and various regions in it
- Atomic versus molecular spectrum
- Absorption versus emission spectrum
- Lambert's law, Beer's law, derivation, verification and deviations of Beer's law
- Concept of transmittance, absorbance and absorptivity
- Numerical problems
- Colorimetry versus spectrophotometry
- Single and double beam instrumentation
- Working of colorimeter and spectrophotometer with simple schematic diagrams
- Application of colorimeter and spectrophotometer in quantitative analysis with reference to estimation of Cu(II) as Cu-ammonia complex
Electromagnetic spectrum and its regions
Electromagnetic radiation travels as waves with wavelength λ and frequency ν (c = λν) and energy E = hν = hc/λ. Shorter wavelength means higher energy.
| Region | Approx. wavelength | Transition caused |
|---|---|---|
| γ-rays | < 0.01 nm | Nuclear |
| X-rays | 0.01–10 nm | Inner-shell electrons |
| Ultraviolet | 10–400 nm (near UV 200–400) | Valence electrons |
| Visible | 400–750 nm | Valence electrons (colour) |
| Infrared | 750 nm–1 mm | Molecular vibrations |
| Microwave | 1 mm–30 cm | Molecular rotations |
| Radio waves | > 30 cm | Nuclear spin (NMR) |
Atomic vs molecular spectrum; absorption vs emission spectrum
- Atomic spectrum: from free atoms; only electronic transitions → sharp lines (e.g. sodium D-lines).
- Molecular spectrum: electronic + vibrational + rotational levels → closely spaced lines merge into bands.
- Absorption spectrum: radiation passed through the sample; dark lines/bands where energy is absorbed (ground → excited state).
- Emission spectrum: excited sample (flame, arc) gives out radiation; bright lines on a dark background (excited → lower state).
Lambert's law, Beer's law and derivation
Lambert's law: when monochromatic light passes through an absorbing medium, the rate of decrease of intensity with thickness is proportional to the intensity: −dI/db = kI.
Beer's law: the rate of decrease of intensity is proportional to the intensity and to the concentration of the absorbing solution: −dI/db = k′Ic.
Derivation (combined): −dI/I = k′c db. Integrating from I0 (b = 0) to I (b = b): ln(I0/I) = k′cb. Converting to log10: log(I0/I) = (k′/2.303)cb = εbc.
Transmittance, absorbance and absorptivity
- Transmittance T = I/I0; %T = 100 × I/I0.
- Absorbance A = log(1/T) = −log T = 2 − log(%T). A has no unit.
- Absorptivity a (c in g L–1) or molar absorptivity ε (c in mol L–1): absorbance of a 1 M solution in a 1 cm cell; a constant for a substance at a given λ.
Verification and deviations of Beer's law
Verification: prepare standard solutions, measure A at λmax and plot A vs c — a straight line through the origin (calibration curve) verifies the law; slope = εb.
Deviations:
- Real: at high concentration (> 0.01 M) molecules interact and refractive index changes; the law holds only for dilute solutions.
- Chemical: association, dissociation, complex formation or reaction with solvent change the absorbing species (e.g. Cr2O72– ⇌ CrO42– with pH).
- Instrumental: non-monochromatic light, stray light, wide slit, unmatched cells.
Numerical problems
Example 1. A solution of ε = 1.5 × 104 L mol–1 cm–1 shows A = 0.45 in a 1 cm cell. Find c and %T.
c = A/(εb) = 0.45/(1.5 × 104 × 1) = 3.0 × 10–5 mol L–1. T = 10–0.45 = 0.355 → %T = 35.5%.
Example 2. A solution transmits 40% of incident light. Find absorbance.
A = −log(0.40) = 0.398 (or 2 − log 40 = 2 − 1.602 = 0.398).
Colorimetry vs spectrophotometry; single and double beam instruments
| Point | Colorimeter | Spectrophotometer |
|---|---|---|
| Wavelength selector | Coloured glass filter (broad band) | Prism or grating monochromator (narrow band) |
| Region | Visible only | UV + visible (often 200–1000 nm) |
| Sample | Must be coloured | Coloured or UV-absorbing |
| Accuracy, cost | Lower, cheap | Higher, costly |
Working of a colorimeter (schematic): light source (tungsten lamp) → lens/slit → filter (colour complementary to the solution) → cuvette with sample → photocell/phototube detector → galvanometer/digital meter reading A or %T. The instrument is set to zero absorbance with the blank (solvent).
Spectrophotometer: source (tungsten for visible, deuterium/hydrogen lamp for UV) → entrance slit → monochromator → exit slit → sample cell (glass for visible, quartz for UV) → detector (photomultiplier) → amplifier and readout.
- Single beam: one light path; blank and sample measured one after the other; simple and cheap, but lamp fluctuations cause error.
- Double beam: a rotating mirror (chopper) splits the beam through reference and sample cells alternately; the ratio is read directly, cancelling source drift; faster scanning of spectra.
Application — estimation of Cu(II) as copper–ammonia complex
- Prepare standard Cu2+ solutions (from CuSO4·5H2O) of known concentration.
- Add excess ammonia to each → deep blue [Cu(NH3)4]2+; dilute to a fixed volume.
- Choose λmax (about 600–620 nm; orange/red filter in a colorimeter) and set zero with a blank (ammonia + water).
- Measure absorbance of standards and plot the calibration curve (A vs concentration).
- Treat the unknown the same way, read its A and find its concentration from the graph.
Likely exam questions
- (Long, 8 marks) State and derive the Beer–Lambert law. Discuss the deviations from Beer's law.
- (Long, 8 marks) Describe the working of a double-beam spectrophotometer with a block diagram. How is Cu(II) estimated colorimetrically?
- (Short, 4 marks) A solution transmits 25% of light in a 1 cm cell. Calculate its absorbance.
- (Short, 4 marks) Distinguish between colorimetry and spectrophotometry.
- (Short, 4 marks) Distinguish between absorption and emission spectra.