Calculator for the Electromagnetic Spectrum
Convert wave length, frequency and energy

| Please enter one value and press the according = button. | ||
| Round to decimal places | ||
| Wave length λ: | * | |
| Frequency f: | * | |
| Photon energy Ep: | * | |
| Energy E: | * | |
| Temperature at λmax: | ||
| Photons per joule: | ||
| Type: | ||
Formulas:
Planck constant h = 6.62606957*10-34 J*s
Speed of light c = 299792458 m/s
c = λ*f
Elektron-volt: 1 eV = 1.602176565*10-19 J
E = h*c / λ
Ep = E / (1.602176565*10-19)
T at λmax = 2,89776829 nm * Kelvin / λ (Wien's displacement law)
T at λmax is the temperature of a black body, whose radiation has a maximum at λ.
Photons per joule = 1 / (1.602176565*10-19 * Ep)
Table:
| Type | Subtype | λ | f | Ep | E |
|---|---|---|---|---|---|
| Low frequency | ELF, extremely low frequency | > 10 Mm | < 30 Hz | < 124 feV | < 1.99*10-32 J |
| SLF, super low frequency | 10 Mm - 1 Mm | 30 Hz - 300 Hz | 124 feV - 1.24 peV | 1.99*10-32 J - 1.99*10-31 J | |
| ULF, ultra low frequency | 1 Mm - 100 km | 300 Hz - 3 kHz | 1.24 peV - 12.4 peV | 1.99*10-31 J - 1.99*10-30 J | |
| VLF, very low frequency | 100 km - 10 km | 3 kHz - 30 kHz | 12.4 peV - 124 peV | 1.99*10-30 J - 1.99*10-29 J | |
| Radio waves | LF, low frequency | 10 km - 650 m | 30 kHz - 461 kHz | 124 peV - 1.91 neV | 1.99*10-29 J - 3.06*10-28 J |
| MF, mid frequency | 650 m - 180 m | 461 kHz - 1.67 MHz | 1.91 neV - 6.89 neV | 3.06*10-28 J - 1.1*10-27 J | |
| HF, high frequency | 180 m - 10 m | 1.67 MHz - 30 MHz | 6.89 neV - 124 neV | 1.1*10-27 J - 1.99*10-26 J | |
| VHF, very high frequency | 10 m - 1 m | 30 MHz - 300 MHz | 124 neV - 1.24 μeV | 1.99*10-26 J - 1.99*10-25 J | |
| Microwaves | UHF, ultra high frequency decimeter band | 1 m - 10 cm | 300 MHz - 3 GHz | 1.24 μeV - 12.4 μeV | 1.99*10-25 J - 2 yJ |
| SHF, super high frequency centimeter band | 10 cm - 1 cm | 3 GHz - 30 GHz | 12.4 μeV - 124 μeV | 1.99 yJ - 19.9 yJ | |
| EHF, extremely high frequency millimeter band | 1 cm - 1 mm | 30 GHz - 300 GHz | 124 μeV - 1.24 meV | 19.9 yJ - 199 yJ | |
| Terahertz radiation | Submillimeter radiation | 1 mm - 100 μm | 300 GHz - 3 THz | 1.24 meV - 12.4 meV | 199 yJ - 1.99 zJ |
| Infrared radiation | Far infrared | 100 μm - 50 μm | 3 THz - 6 THz | 12.4 meV - 24.8 meV | 1.99 zJ - 3.97 zJ |
| Mid infrared | 50 μm - 3 μm | 6 THz - 100 THz | 24.8 meV - 413 meV | 3.97 zJ - 66.2 zJ | |
| Near infrared | 3 μm - 780 nm | 100 THz - 384 THz | 413 meV - 1.59 eV | 66.2 zJ - 255 zJ | |
| Visible light | Red | 780 nm - 640 nm | 384 THz - 468 THz | 1.59 eV - 1.94 eV | 255 zJ - 310 zJ |
| Orange | 640 nm - 600 nm | 468 THz - 500 THz | 1.94 eV - 2.07 eV | 310 zJ - 331 zJ | |
| Yellow | 600 nm - 570 nm | 500 THz - 526 THz | 2.07 eV - 2.18 | 331 zJ - 349 zJ | |
| Green | 570 nm - 490 nm | 526 THz - 612 THz | 2.18 eV - 2.53 eV | 349 zJ - 405 zJ | |
| Blue | 490 nm - 430 nm | 612 THz - 697 THz | 2.53 eV - 2.88 eV | 405 zJ - 462 zJ | |
| Violet | 430 nm - 380 nm | 697 THz - 789 THz | 2.88 eV - 3.26 eV | 462 zJ - 523 zJ | |
| Ultraviolet | Near UV, UVA | 380 nm - 315 nm | 789 THz - 952 THz | 3.26 eV - 3.94 eV | 523 zJ - 631 zJ |
| Near UV, UVB | 315 nm - 280 nm | 952 THz - 1.07 PHz | 3.94 eV - 4.43 eV | 631 zJ - 709 zJ | |
| Near UV, UVC | 280 nm - 200 nm | 1.07 PHz - 1.5 PHz | 4.43 eV - 6.2 eV | 709 zJ - 993 zJ | |
| Far ultraviolet | 200 nm - 50 nm | 1.5 PHz - 6 PHz | 6.2 eV - 24.8 eV | 993 zJ - 3.97 aJ | |
| XUV, EUV, extreme UV | 50 nm - 1 nm | 6 PHz - 300 PHz | 24.8 eV - 1.24 keV | 3.97 aJ - 199 aJ | |
| X-radiation | Soft X-rays, SX | 1 nm - 100 pm | 300 PHz - 3 EHz | 1.24 keV - 12.4 keV | 199 aJ - 1.99 fJ |
| Hard X-rays, HX | 100 pm - 10 pm | 3 EHz - 30 EHz | 12.4 keV - 124 keV | 1.99 fJ - 19.9 fJ | |
| Gamma radiation | γ | < 10 pm | > 30 EHz | > 124 keV | > 19.9 fJ |
| Cosmic γ-rays | < 4 pm | > 75 EHz | > 310 keV | > 49.7 fJ |
The electromagnetic spectrum is the region in which electromagnetic waves occur. The different waves differ in their wavelength, i.e. the distance between two wave crests, and their frequency, the number of times a wave crest is passed through per second. Since electromagnetic waves in the same medium all have the same speed, namely the speed of light, both values can be converted directly into one another, as can the energy that such a wave has. The electromagnetic waves that we are most familiar with are those of light, because we have sensory organs to perceive them. However, light only takes up a tiny part of the electromagnetic spectrum. We also notice infrared radiation when we get warm, but our ability to perceive it is much less precise here. We only notice other types of radiation when they harm us or have already harmed us, such as ultraviolet, which causes sunburn. The shorter the wavelength (and of course the more intense, i.e. the more waves), the more dangerous the radiation is for us.
Radiation can be seen not only as a wave, but also as a particle. The radiation particles are called photons. Which perspective is appropriate really depends on the case, and we have now become accustomed to the wave-particle duality, which occurs not only with electromagnetic waves, but also with electrons, for example. This is just one of the many aspects of quantum mechanics that are not particularly understandable. In fact, quantum mechanics very often runs counter to what seems to be common sense, but it simply works very well and provides predictions and explanations for real phenomena in the nature of the very small that cannot be explained without it. Physical theories that do not require quantum mechanics are called classical theories. One of these is the general theory of relativity, which also provides very good predictions and explanations, but for the area of the very large. Both important theories contradict each other where they meet. These are particularly black holes and singularities, where the very large and the very small coincide. However, there are certainly promising attempts to bring the two theories closer together.
Last updated on 06/23/2025. Author: Jürgen Kummer
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