Cosmology · Light, redshift and first distance clues
Light and wavelength beyond visible colours
A radio signal and visible starlight belong to the same physical family. Learn what wavelength measures, how it relates to frequency, and why a wave drawing is not a picture of a photon's path.
Preparation: ratios, powers of ten and ordinary arithmetic. Physical quantities and notation are introduced as they are needed.
Back to the chapterAfter reading, you can
- Distinguish wavelength, frequency and wave amplitude.
- Convert a supplied vacuum wavelength into a frequency with consistent units.
- Explain what a telescope's choice of wavelength reveals and leaves unmeasured.
Measure the spacing before naming the colour
Imagine a repeating pattern drawn along a ruler. The distance from one crest to the next is one wavelength, written λ, the Greek letter lambda. Wavelength is a length. Frequency, written ν, the Greek letter nu, counts how many cycles pass a fixed location each second. One cycle per second is one hertz, abbreviated Hz.
These definitions answer different questions: how far apart is the pattern, and how often does it repeat at the detector? A snapshot along a ruler concerns wavelength. A recording over time at one place concerns frequency. Neither quantity is the height of the drawn wave.
For electromagnetic radiation the oscillating quantities are electric and magnetic fields. A sinusoidal curve can represent one field component along a chosen direction at an instant. Its vertical axis represents a field value, not the up-and-down position of a tiny travelling particle. The curve is a model of a field, rather than a photograph of a photon weaving through space. For a sinusoidal field varying about zero, its amplitude is the maximum magnitude of that field component: the distance from the middle line to a crest on this field-value graph. Its unit belongs to the field, not to a length travelled by a particle.
One vacuum speed connects the two measurements
In vacuum, local propagation obeys c = λν. The same cycle that occupies length λ passes in time 1/ν, so dividing that length by that time gives λν. Here c is the vacuum speed of light, exactly 299,792,458 metres per second in SI. For rounded teaching calculations we may state c ≈ 3.00 × 10⁸ m/s.
If the spacing doubles while propagation speed stays the same, half as many cycles pass each second. Wavelength and frequency therefore vary inversely. A longer wavelength does not mean the light travels more slowly in vacuum. Propagation through matter is a separate problem: the material response can depend on frequency, and a vacuum formula should not be silently applied with the wrong speed.
At a chosen vacuum wavelength of 600 nm, first convert nanometres into metres: 600 nm = 6.00 × 10⁻⁷ m. Then ν = c/λ ≈ (3.00 × 10⁸ m/s)/(6.00 × 10⁻⁷ m) = 5.00 × 10¹⁴ s⁻¹. The metre cancels. The reciprocal second is the frequency unit Hz. Using the exact c gives about 4.9965 × 10¹⁴ Hz; the rounded answer reflects the stated approximation.
| Wavelength | In metres | Frequency |
|---|---|---|
| 600 nm | 6.00 × 10⁻⁷ m | 5.00 × 10¹⁴ Hz |
| 1 mm | 1.00 × 10⁻³ m | 3.00 × 10¹¹ Hz |
| 1 nm | 1.00 × 10⁻⁹ m | 3.00 × 10¹⁷ Hz |
Visible colour is one small part of the family
Radio waves, microwaves, infrared, visible light, ultraviolet, X-rays and gamma rays are forms of electromagnetic radiation. The names divide useful ranges; they do not describe different vacuum speed limits. The boundaries between some named ranges are conventional, and X-rays and gamma rays are also often distinguished by their production processes.
Our eyes respond to a limited range. A detector can instead measure radiation outside that range, converting its response into an electrical signal. Assigning visible colours to an infrared or radio image can help display measurements, but those display colours need a key. They are not a claim that the unaided eye would see those colours at the source.
A source generally emits a distribution of wavelengths. A telescope image taken through one filter records only part of that distribution, weighted by the filter and detector response. A source absent in that band need not be absent altogether. Comparing bands can reveal a different component or an intervening effect; interpreting it still needs a physical model.
Energy per photon and amount of light are different
Light also exchanges energy in quanta called photons. The photon energy is E = hν, where h is Planck's constant. Thus shorter vacuum wavelength corresponds to higher frequency and higher energy per photon. This is a relationship between measured properties, not a request to imagine a photon as a classical bead with a miniature sinusoid attached.
The energy of one photon does not tell you the total power arriving at a detector. That also depends on how many photons arrive, their energies, the collecting area and the time interval. A faint high-frequency source can deliver less total energy per second than a bright low-frequency source. Wave amplitude, frequency and total received power should not be used as interchangeable words.
For two photons whose frequencies differ by a factor of three, their energies differ by that same factor. If the second stream contains only one tenth as many such photons per second as the first, its total photon energy delivered per second is three tenths as large, provided the comparison uses the same collecting area. Ratios can clarify a measurement before any large numerical constants are needed.
Turn the definitions into a check
Suppose a reported vacuum wave doubles both its wavelength and frequency while retaining the same c. Their product would increase by four, contradicting c = λν. Check units, conventions and which propagation medium was intended before inventing a new physical interpretation.
For cosmology, the key next step is comparing a received wavelength with a reference wavelength for an identified spectral feature. A longer measured wavelength is a comparison of radiation properties at different events. It does not, by itself, reveal a distance or choose among motion, gravitational and cosmological interpretations. The next lessons build that inference one step at a time.
Worked reasoning
Predict before calculating
A chosen vacuum signal changes from wavelength 1 mm to 0.5 mm. How do its frequency and photon energy compare?
- At fixed c, ν = c/λ, so halving λ doubles ν.
- With rounded c, the frequencies are 3.00 × 10¹¹ Hz and 6.00 × 10¹¹ Hz.
- E = hν gives twice the energy per photon. It gives no photon arrival rate.
Frequency and energy per photon both double; the total received power remains unspecified.
Try the reasoning
A label says wavelength = 20 Hz. What is wrong with its unit?
Show the answer and reasoning
Hz measures frequency, not wavelength.
Wavelength requires a length unit such as metres or nanometres. Frequency counts cycles per second.
Using rounded c, what vacuum frequency corresponds to 300 nm?
Show the answer and reasoning
1.00 × 10¹⁵ Hz.
300 nm = 3.00 × 10⁻⁷ m. Dividing 3.00 × 10⁸ m/s by this length gives 1.00 × 10¹⁵ s⁻¹.
Does a sinusoidal field-versus-position graph show a photon travelling farther by following the drawn wiggles?
Show the answer and reasoning
No.
The vertical coordinate is a field value. Treating it as transverse particle displacement changes what the graph represents.
What to carry forward
- Wavelength is a spacing; frequency is a repetition rate.
- In vacuum, λν = c, so longer wavelength means lower frequency.
- Electromagnetic radiation extends beyond visible colours.
- Photon energy, photon arrival rate and total received power answer different questions.
References
Sources supporting the explanations, physical distinctions and examples in this lesson.
- Definitions of SI Base UnitsNational Institute of Standards and TechnologyTeaching resource
Andrew Fraknoi; David Morrison; Sidney C. Wolff3 sources
- Astronomy 2e, 5.1: The Behavior of LightAndrew Fraknoi; David Morrison; Sidney C. WolffTeaching resource
- Astronomy 2e, 5.2: The Electromagnetic SpectrumAndrew Fraknoi; David Morrison; Sidney C. WolffTeaching resource
- Astronomy 2e, 5.6: The Doppler EffectAndrew Fraknoi; David Morrison; Sidney C. WolffTeaching resource
- The Electromagnetic SpectrumNASA Goddard Imagine the Universe teamTeaching resource
- What Is Ionizing Radiation? — basic types subsectionAdvisory Committee on Human Radiation Experiments; U.S. Department of Energy archiveTeaching resource
- Cosmology, Section 1: The Expanding UniverseDavid TongCourse notes
- Distance measures in cosmology, sections 3 and 7David W. HoggTeaching resource
- Gravitational redshift and White Dwarf starsVirginia Trimble; Martin BarstowTeaching resource