Light and the electromagnetic spectrum: wavelength, UV and absorbance
The electromagnetic spectrum in order, from radio waves to gamma rays: how wavelength, frequency and energy link, and why peptides are measured with UV light.
By Zachery Casey · Published · Reviewed · Editorial policy
The electromagnetic spectrum is the full range of electromagnetic radiation, ordered by wavelength from radio waves to gamma rays. Visible light is the narrow band from about 380 to 700 nm. Many lab measurements are really measurements of light. An HPLC detector shines ultraviolet light through the liquid leaving the column. A spectrophotometer measures how much light a solution absorbs. Infrared, Raman and fluorescence spectroscopy each use a different part of the spectrum. This guide explains what wavelength means, how the electromagnetic spectrum is laid out, why peptides are measured in the ultraviolet, and what an absorbance number tells you.
Terms are defined in the glossary.
What is wavelength?
Light travels as a wave of electric and magnetic fields. The wavelength is the distance from one peak of the wave to the next. It is written with the Greek letter λ (lambda).
Three properties are linked:
- Wavelength (λ): the length of one wave, usually given in nanometres (nm) for light. One nanometre is a millionth of a millimetre.
- Frequency (f, sometimes written ν): how many waves pass a point each second, in hertz (Hz).
- Energy: how much energy each packet of light, or photon, carries.
Because all light travels at the same speed, a shorter wavelength means a higher frequency and more energy per photon. Ultraviolet light carries more energy than visible light, and visible light more than infrared. That is why ultraviolet light can break chemical bonds and infrared light mostly warms things.
The wave equation: c = fλ and E = hf
Two short equations tie the three properties together:
- c = fλ. The speed of light (c) equals frequency times wavelength. Since c is fixed at 299,792,458 m/s (BIPM, SI Brochure), knowing one of f or λ gives the other.
- E = hf. The energy of one photon (E) equals the Planck constant (h) times the frequency. The Planck constant is exactly 6.626 070 15 × 10⁻³⁴ J s (NIST, CODATA).
A worked example: ultraviolet light at 220 nm, a wavelength used to detect peptides in HPLC.
- Convert the wavelength to metres: 220 nm = 220 × 10⁻⁹ m.
- Frequency: f = c ÷ λ = 299,792,458 ÷ (220 × 10⁻⁹) ≈ 1.36 × 10¹⁵ Hz.
- Energy of one photon: E = hf = 6.626 × 10⁻³⁴ × 1.36 × 10¹⁵ ≈ 9.03 × 10⁻¹⁹ J.
- For a mole of photons, multiply by the Avogadro constant (6.022 × 10²³): about 544 kJ per mole.
Halve the wavelength and the frequency and energy double. Infrared light at 6,000 nm (a wavenumber of about 1,667 cm⁻¹) has under a twenty-fifth of the energy per photon of the 220 nm light.
In infrared spectroscopy, light is often described by wavenumber instead: the number of waves per centimetre, in cm⁻¹. A higher wavenumber means a shorter wavelength. See reading an IR spectrum.
The electromagnetic spectrum
All electromagnetic radiation is the same kind of wave. Only the wavelength differs.
The electromagnetic spectrum in order
From the longest wavelength (lowest frequency and energy) to the shortest (highest frequency and energy):
- Radio waves
- Microwaves
- Infrared
- Visible light (red, orange, yellow, green, blue, violet)
- Ultraviolet
- X-rays
- Gamma rays
The table gives rough ranges. The frequencies are worked out from the wavelengths with c = fλ.
| Region | Rough wavelength | Rough frequency | What it does to molecules | Lab method |
|---|---|---|---|---|
| Radio waves | Metres and longer | Below about 3 × 10⁸ Hz | Flips the spin of atomic nuclei in a strong magnet | NMR spectroscopy |
| Microwaves | Millimetres to about 30 cm | About 10⁹ to 3 × 10¹¹ Hz | Makes molecules rotate | Microwave heating |
| Infrared | About 700 nm to 1 mm | About 3 × 10¹¹ to 4.3 × 10¹⁴ Hz | Makes bonds stretch and bend | FTIR |
| Visible | About 380–700 nm | About 4.3 × 10¹⁴ to 7.9 × 10¹⁴ Hz | Moves electrons in coloured compounds | Colorimetric assays; the blue of GHK-Cu |
| Ultraviolet | About 10–400 nm | About 7.5 × 10¹⁴ to 3 × 10¹⁶ Hz | Moves electrons in bonds and ring systems | UV detection in HPLC, A280 |
| X-rays | About 0.01–10 nm | About 3 × 10¹⁶ to 3 × 10¹⁹ Hz | Scattered by electrons in a crystal | X-ray crystallography |
| Gamma rays | Shorter still | Above about 3 × 10¹⁹ Hz | Breaks bonds and ionises atoms | Sterilising some plastic labware |
The boundaries are conventions, and sources draw them slightly differently. The human eye typically detects about 380 to 700 nm (NASA). Raman spectroscopy uses a visible or near-infrared laser but reads the same bond vibrations as infrared.
The ultraviolet bands
Ultraviolet light is often split into three bands (WHO):
- UV-A: 315–400 nm
- UV-B: 280–315 nm
- UV-C: 100–280 nm
Below about 200 nm, oxygen in the air absorbs strongly. This region is called the vacuum or far ultraviolet, and instruments working there are flushed with nitrogen.
Why peptides are measured with ultraviolet light
Most peptides are colourless: they don't absorb visible light. They do absorb ultraviolet light, at two main places.
| Wavelength | What absorbs | Used for |
|---|---|---|
| About 205–220 nm | The peptide bond in the backbone, plus some side chains | HPLC detection of every peptide; far-UV concentration measurement |
| About 280 nm | Tryptophan and tyrosine side chains, and disulfide bonds | Concentration of peptides that contain these residues |
Because every peptide has peptide bonds, detection at 214–220 nm sees almost every peptide-related species in an HPLC run. That is why it is the usual wavelength for purity testing. See how HPLC works. At 280 nm, a peptide without tryptophan or tyrosine is almost invisible. See measuring peptide concentration.
The trade-off of working at short wavelengths is that many other things absorb there too, including some solvents, buffers and dissolved oxygen. That is why HPLC solvents are chosen for their UV cut-off, the wavelength below which they absorb too much to use. See HPLC and LC-MS solvents.
What is a spectrophotometer?
A spectrophotometer measures how much light a sample absorbs at a chosen wavelength. What makes it a spectrophotometer is the monochromator, the part that picks out one wavelength from the light source (LibreTexts, Instrumentation). It has four main parts:
- A light source.
- A monochromator, which selects the wavelength. Scanning through wavelengths records a whole spectrum.
- A sample holder for the cuvette, in a light-tight compartment.
- A detector, which measures the light that gets through.
A single-beam instrument measures the blank and the sample one after the other. A double-beam instrument switches the light between them continuously, which corrects for drift in the lamp and detector (LibreTexts). An instrument covering both the ultraviolet and visible ranges is called a UV-Vis spectrophotometer, and the method UV-Vis spectroscopy. HPLC UV detectors work on the same principle, with a flow cell in place of the cuvette.
What is absorbance?
A spectrophotometer shines light of one wavelength through a sample and measures how much comes out the other side. Transmittance is the fraction that gets through. Absorbance turns that into a more convenient number:
A = log₁₀(I₀ ÷ I)
where I₀ is the light going in and I is the light coming out.
| Absorbance | Light transmitted |
|---|---|
| 0 | 100% |
| 0.3 | About 50% |
| 1 | 10% |
| 2 | 1% |
| 3 | 0.1% |
Absorbance has no units. Because it is a logarithm, each step of 1 cuts the light reaching the detector tenfold. At high absorbance so little light gets through that stray light and detector noise dominate, so readings are most reliable in the lower part of the range. A concentrated sample is diluted to bring it down.
Absorbance rises in proportion to concentration and to the distance the light travels through the sample. That relationship is the Beer–Lambert law, covered in measuring peptide concentration and the Beer–Lambert calculator.
Cuvettes and wavelength
The container matters too. Ordinary glass and most plastics absorb ultraviolet light, so a sample measured at 280 nm or below needs a quartz cuvette or a plastic one sold as UV-transparent. Each reading is taken against a blank: the same cuvette filled with solvent only, so the solvent's own absorbance is subtracted.
Other molecules measured in the ultraviolet
The same approach works for any compound with a UV-absorbing group. The adenine ring of NAD+ absorbs at 260 nm, and its reduced form NADH has a second band at 340 nm, which is how the two are told apart. See NAD+ structure and stability.
Light and stored samples
The same energy that makes ultraviolet light useful for measuring also lets it damage molecules. Tryptophan, tyrosine and phenylalanine absorb ultraviolet light and can break down as a result. Amber glass blocks most ultraviolet and blue light, and a closed box blocks it all. See how to store freeze-dried (lyophilised) peptides.
Fluorescence: light in, different light out
Some molecules give out light after absorbing it, at a longer wavelength. This is fluorescence. Tryptophan absorbs near 280 nm and fluoresces around 350 nm. Measuring the emitted light is far more sensitive than measuring absorbance. See NMR, FTIR and other methods.
Related guides
For reading the trace a UV detector produces, see reading a chromatogram. For the extinction coefficient at 205 and 280 nm, use the extinction coefficient calculator. An independent lab tests every lot we sell for purity by HPLC and identity by mass spectrometry. Every lot has its own COA, published on the product page and on that lot's own page. See Quality.
More on how the tests work
- Reading a chromatogram: peaks, baseline, signal-to-noise and calibration curvesWhat a chromatogram is and how to read one: retention time, peak area, signal-to-noise ratio and detection limits, plus how a calibration curve works.
- Reading impurity peaks: what +16, +1 and −18 Da meanHow peptide impurities show up on HPLC and mass spectrometry: oxidation, deamidation, aspartimide, deletions and leftover protecting groups, by mass shift.
- Mass spectrometry and peptide identity confirmationWhat mass spectrometry is, how it works, and how it confirms a peptide's identity: charge states, monoisotopic vs average mass, and what a match proves.