{"id":2115,"date":"2026-10-01T13:22:31","date_gmt":"2026-10-01T13:22:31","guid":{"rendered":"https:\/\/physicsfundamentalsinfo.com\/blog\/?p=2115"},"modified":"2026-10-01T13:22:33","modified_gmt":"2026-10-01T13:22:33","slug":"ultraviolet-radiation","status":"publish","type":"post","link":"https:\/\/physicsfundamentalsinfo.com\/blog\/waves\/ultraviolet-radiation\/","title":{"rendered":"Ultraviolet Radiation: Types &#038; Effects"},"content":{"rendered":"\n<div class=\"pf-citation\"><div class=\"eyebrow\">Definition<\/div><p>\n\nUltraviolet radiation is the 100 to 400 nm region of the electromagnetic spectrum, invisible light just beyond violet, whose photons carry between 3.0996 and 12.3984 eV. Convention divides it into three bands: UVA at 315 to 400 nm, UVB at 280 to 315 nm and UVC at 100 to 280 nm. Photon energy is hc divided by wavelength.\n\n<\/p><\/div>\n\n<p>Stand outside on a clear day and something is landing on you that you cannot see and cannot feel. You find out about it hours later, when the back of your neck starts to sting.<\/p>\n\n<p>The strange part is how small the step is. At 400 nm the longest ultraviolet and the deepest violet the eye can catch carry exactly the same 3.0996 eV, yet everything shorter than that line gets filed as radiation and everything longer as light. This page follows the physics across the line: the three bands, what each photon carries, which of them reaches the ground, and where the tidy picture stops being true.<\/p>\n\n<h2>What Is Ultraviolet Radiation?<\/h2>\n\n<p>Ultraviolet radiation is electromagnetic radiation with a wavelength between 100 and 400 nm: shorter than violet light, longer than X-rays, and invisible because the eye carries no receptor that responds below about 400 nm.<\/p>\n\n<p>The name describes a position, not a property. Violet is the shortest wavelength a person can register, and ultra-violet is whatever lies past it. Nothing about the wave itself changes at that point \u2014 it is the same oscillating electric and magnetic field that carries a radio broadcast, differing only in wavelength.<\/p>\n\n<p>Wavelength is what decides how much energy each photon delivers, and that single fact drives everything else on this page. Longer waves hand over less per photon; shorter waves hand over more. Our guide to the <a href=\"https:\/\/physicsfundamentalsinfo.com\/blog\/waves\/electromagnetic-spectrum\/\">electromagnetic spectrum<\/a> lays out the full run of bands that ultraviolet sits inside.<\/p>\n\n<p>What earns ultraviolet its own page is where it sits. It occupies the stretch where photon energies become big enough to rearrange molecules but stay below the energies that strip electrons off atoms outright \u2014 a narrow strip, and almost every practical fact about UV follows from it.<\/p>\n\n<p>One habit is worth picking up straight away. If a lamp, a warning label or a study says only &#8220;UV&#8221;, the description is incomplete: a 365 nm black light and a 254 nm germicidal tube are both ultraviolet, and they do entirely different things to whatever is in front of them.<\/p>\n\n<h2>The Ultraviolet Radiation Formula: Energy from Wavelength<\/h2>\n\n<p>A photon&#8217;s energy is the Planck constant multiplied by the speed of light, divided by its wavelength.<\/p>\n\n<div class=\"pf-formula\">E = h \u00b7 c \/ \u03bb<\/div>\n\n<ul>\n<li><strong>E<\/strong> \u2014 the photon energy, in joules (J). Quoted in electronvolts (eV) on this page, where 1 eV = 1.602176634 \u00d7 10<sup>\u221219<\/sup> J.<\/li>\n<li><strong>h<\/strong> \u2014 the Planck constant, 6.62607015 \u00d7 10<sup>\u221234<\/sup> J\u00b7s, exact by definition since 2019.<\/li>\n<li><strong>c<\/strong> \u2014 the speed of light in vacuum, 299,792,458 m\/s, also exact by definition.<\/li>\n<li><strong>\u03bb<\/strong> \u2014 the wavelength, in metres (m). Ultraviolet is quoted in nanometres by universal habit, and 1 nm = 10<sup>\u22129<\/sup> m.<\/li>\n<\/ul>\n\n<p>Nobody works it in those units. Fold the constants together, divide through by the charge on an electron and measure the wavelength in nanometres, and the whole thing collapses to one division: the energy in electronvolts is 1239.842 divided by the wavelength in nanometres. If you would rather not divide, our <a href=\"https:\/\/physicsfundamentalsinfo.com\/calculators\/ultraviolet-radiation\">ultraviolet radiation calculator<\/a> takes a wavelength, an energy or a frequency and returns the other two with the band named.<\/p>\n\n<p>Why a photon&#8217;s energy should depend on its frequency at all is a separate question, and it is answered in our <a href=\"https:\/\/physicsfundamentalsinfo.com\/blog\/modern-physics\/photon-energy-formula\/\">photon energy formula<\/a> guide. Here the relation is a tool. It gets used, not re-derived.<\/p>\n\n<p>Worth committing to memory in place of the formula: multiply any photon&#8217;s energy in electronvolts by its wavelength in nanometres and you get 1239.842, every single time. It turns checking somebody else&#8217;s figures into a two-second job.<\/p>\n\n<div class=\"pf-table-scroll\" style=\"display:block;width:100%;max-width:100%;overflow-x:auto;-webkit-overflow-scrolling:touch;margin:1.5em 0;\">\n<table style=\"width:100%;border-collapse:collapse;word-break:break-word;\">\n<thead>\n<tr><th style=\"text-align:left;padding:8px 10px;border-bottom:2px solid #C8932A;font-weight:700;white-space:nowrap;\">Wavelength (nm)<\/th><th style=\"text-align:left;padding:8px 10px;border-bottom:2px solid #C8932A;font-weight:700;white-space:nowrap;\">Photon energy (eV)<\/th><th style=\"text-align:left;padding:8px 10px;border-bottom:2px solid #C8932A;font-weight:700;white-space:nowrap;\">Photon energy (J)<\/th><th style=\"text-align:left;padding:8px 10px;border-bottom:2px solid #C8932A;font-weight:700;white-space:nowrap;\">Frequency (Hz)<\/th><th style=\"text-align:left;padding:8px 10px;border-bottom:2px solid #C8932A;font-weight:700;white-space:nowrap;\">Band<\/th><th style=\"text-align:left;padding:8px 10px;border-bottom:2px solid #C8932A;font-weight:700;white-space:nowrap;\">Energy (kJ\/mol)<\/th><\/tr>\n<\/thead>\n<tbody>\n<tr><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">100<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">12.3984<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">1.9864 \u00d7 10<sup>\u221218<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">2.9979 \u00d7 10<sup>15<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">UVC<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">1196.3<\/td><\/tr>\n<tr><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">180<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">6.8880<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">1.1036 \u00d7 10<sup>\u221218<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">1.6655 \u00d7 10<sup>15<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">UVC<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">664.6<\/td><\/tr>\n<tr><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">200<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">6.1992<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">9.9322 \u00d7 10<sup>\u221219<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">1.4990 \u00d7 10<sup>15<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">UVC<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">598.1<\/td><\/tr>\n<tr><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">254<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">4.8813<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">7.8207 \u00d7 10<sup>\u221219<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">1.1803 \u00d7 10<sup>15<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">UVC<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">471.0<\/td><\/tr>\n<tr><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">280<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">4.4280<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">7.0944 \u00d7 10<sup>\u221219<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">1.0707 \u00d7 10<sup>15<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">UVB<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">427.2<\/td><\/tr>\n<tr><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">300<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">4.1328<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">6.6215 \u00d7 10<sup>\u221219<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">9.9931 \u00d7 10<sup>14<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">UVB<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">398.8<\/td><\/tr>\n<tr><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">315<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">3.9360<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">6.3062 \u00d7 10<sup>\u221219<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">9.5172 \u00d7 10<sup>14<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">UVA<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">379.8<\/td><\/tr>\n<tr><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">365<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">3.3968<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">5.4423 \u00d7 10<sup>\u221219<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">8.2135 \u00d7 10<sup>14<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">UVA<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">327.7<\/td><\/tr>\n<tr><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">400<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">3.0996<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">4.9661 \u00d7 10<sup>\u221219<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">7.4948 \u00d7 10<sup>14<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">UVA<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">299.1<\/td><\/tr>\n<tr><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">550<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">2.2543<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">3.6117 \u00d7 10<sup>\u221219<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">5.4508 \u00d7 10<sup>14<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">Not UV (green light)<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">217.5<\/td><\/tr>\n<tr><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">700<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">1.7712<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">2.8378 \u00d7 10<sup>\u221219<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">4.2827 \u00d7 10<sup>14<\/sup><\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">Not UV (red light)<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">170.9<\/td><\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n\n<p>The last two rows are green and red light, and they are in the table deliberately. They are the comparison the rest of this page keeps returning to. The Band column uses the three divisions set out in the next section.<\/p>\n\n<p>Read the energy column downwards and the shape of the relation is unmistakable. The 100 nm end of ultraviolet carries exactly four times the energy of the 400 nm end, 12.3984 eV against 3.0996 eV, because a quarter of the wavelength means four times the energy.<\/p>\n\n<p>The lab below puts that single division on a slider. Drag one wavelength between 100 and 400 nm and watch the photon energy, the band name and the effect on a chosen metal move together.<\/p>\n\n<div class=\"pf-sim-slot\"><div class=\"pf-sim-slot-header\"><span class=\"icon-dot\"><\/span><span class=\"label\">Ultraviolet Radiation Lab<\/span><\/div><div class=\"pf-sim-slot-body\"><style>.pf-sim-frame{width:100%;border:none;height:600px}@media(max-width:760px){.pf-sim-frame{height:1000px}}<\/style><iframe src=\"\/labs\/ultraviolet-radiation.html?embed=1\" class=\"pf-sim-frame\" loading=\"lazy\"><\/iframe><\/div><\/div>\n\n<h2>UVA, UVB and UVC: Who Drew the Lines, and Where<\/h2>\n\n<p>The <a href=\"https:\/\/www.who.int\/news-room\/questions-and-answers\/item\/radiation-ultraviolet-(uv)\" target=\"_blank\" rel=\"noopener\">World Health Organization<\/a> splits the ultraviolet range into UVA at 315 to 400 nm, UVB at 280 to 315 nm and UVC at 100 to 280 nm.<\/p>\n\n<p>Those three numbers are an agreement, not a discovery. Nothing measurable changes as a wave crosses 315.0 nm; the atmospheric absorption and the biological response that the boundaries stand for both vary smoothly through the range, and another committee could reasonably have put the lines a few nanometres away. They are vocabulary \u2014 extremely useful vocabulary, but vocabulary.<\/p>\n\n<p>Any convention still needs a rule for its own edges, or two sources will file 280 nm differently. On this page, and in the lab and calculator built alongside it, each band owns its short edge and not its long one. So 280 nm counts as UVB, 315 nm counts as UVA, and 400 nm is the last wavelength that is ultraviolet at all.<\/p>\n\n<figure style=\"margin:32px auto;max-width:720px;text-align:center;\">\n  <img src=\"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-content\/uploads\/2026\/09\/ultraviolet-radiation-diagram-01-768x399.jpg\" srcset=\"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-content\/uploads\/2026\/09\/ultraviolet-radiation-diagram-01-768x399.jpg 768w, https:\/\/physicsfundamentalsinfo.com\/blog\/wp-content\/uploads\/2026\/09\/ultraviolet-radiation-diagram-01.jpg 1400w\" sizes=\"auto, (max-width: 760px) 100vw, 720px\" width=\"1400\" height=\"728\" alt=\"A single linear wavelength axis from 100 to 400 nanometres carrying the three ultraviolet bands as one filled strip. The strip is divided at 280 and 315 nanometres: UVC fills 100 to 280 nm in wine, UVB fills the narrow 280 to 315 nm slot in gold, and UVA fills 315 to 400 nm in pale grey. Each band carries its name alone, UVC, UVB or UVA; no range is written inside the bands, and the ranges are read instead off the numbered ticks at 100, 280, 315 and 400 along the axis beneath the strip. Two dashed vertical rules stand on the same axis at the photoelectric thresholds of two metals, labelled above the strip as Cu threshold 263.80 nm, inside UVC, and Zn threshold 288.34 nm, inside UVB. Each rule is wine above the strip and changes colour where it crosses the band, to cream over UVC and to navy over UVB. A gold bar beneath the axis runs from 100 nm to 288.34 nm and is labelled as the wavelengths short enough to free an electron from zinc. Notes beneath state that the sodium threshold at 539.06 nm and the caesium threshold at 590.40 nm lie beyond the right-hand edge of this axis, in visible light, and that the 280 and 315 nm divisions are a World Health Organization convention rather than a physical edge.\" loading=\"lazy\" decoding=\"async\" style=\"width:100%;height:auto;border-radius:4px;\">\n  <figcaption style=\"font-size:13px;color:#1F2E47;font-style:italic;margin-top:8px;\">The three bands on one linear wavelength axis, with two photoelectric thresholds drawn on the same scale. UVB occupies a strikingly narrow slot; the caesium and sodium thresholds fall off the right-hand edge entirely, because they lie in visible light.<\/figcaption>\n<\/figure>\n\n<p>Two extra markers sit on that axis, and they belong to a section further down: they are the wavelengths at which copper and zinc give up an electron. They are drawn here because the whole value of a single linear axis is that everything has to live on it.<\/p>\n\n<p>Draw the bands to scale and one thing jumps out. UVB is a sliver, 35 nm wide, squeezed between a UVC band of 180 nm and a UVA band of 85 nm \u2014 yet that sliver does most of the biological work at ground level.<\/p>\n\n<p>In photon energy the gap is wider still, not narrower. UVC covers 7.9704 eV, from 4.4280 up to 12.3984; UVB covers 0.4920 eV and UVA 0.8364 eV. So UVC is a little over five times UVB&#8217;s width in nanometres and 16.2 times its width in electronvolts \u2014 equal steps in wavelength are never equal steps in energy, because one goes as the reciprocal of the other.<\/p>\n\n<h2>Which Types of UV Reach the Ground?<\/h2>\n\n<p>UVA reaches the surface, most UVB does not, and UVC never does at all, because the atmosphere removes the shortest wavelengths first and removes them most completely.<\/p>\n\n<p>WHO states the split plainly. UVA accounts for approximately 95 per cent of the ultraviolet arriving at the Earth&#8217;s surface; most solar UVB is filtered out on the way down; and UVC is filtered completely, so none of it reaches the ground. Four gases in the air above you do the absorbing: ozone, water vapour, oxygen and carbon dioxide.<\/p>\n\n<p>Line that up against the band edges and the pattern is exactly the one the energy column predicts. The more energy a photon carries, the more readily something in the atmosphere absorbs it \u2014 which is a large part of why the bands were drawn where they were in the first place.<\/p>\n\n<p>There is a practical consequence hiding in it. The germicidal wavelength every microbiology laboratory relies on, 254 nm, is UVC, so no amount of standing in sunlight will ever supply it. That wavelength has to be manufactured, and a lamp that makes it is doing something sunlight at ground level simply cannot.<\/p>\n\n<p>Ozone is the piece of this that moves. Because it controls how much UVB gets through, the ozone column overhead is watched continuously from orbit: <a href=\"https:\/\/science.nasa.gov\/ems\/10_ultravioletwaves\/\" target=\"_blank\" rel=\"noopener\">NASA&#8217;s page on ultraviolet waves<\/a> describes the Ozone Monitoring Instrument aboard the Aura satellite, which maps atmospheric ozone in Dobson Units so the ultraviolet arriving at the surface can be estimated.<\/p>\n\n<figure style=\"margin:32px auto;max-width:640px;text-align:center;\">\n  <img decoding=\"async\" src=\"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-content\/uploads\/2026\/10\/the-Antarctic-ozone-hole-seen-from-orbit.jpg\"\n       alt=\"Satellite map of atmospheric ozone over Antarctica in Dobson Units, the thinned ozone column that lets more ultraviolet radiation reach the surface\"\n       loading=\"lazy\"\n       style=\"width:100%;height:auto;border-radius:4px;\" width=\"1920\" height=\"1280\">\n  <figcaption style=\"font-size:13px;color:#1F2E47;font-style:italic;margin-top:8px;\">Ozone measured from orbit in Dobson Units. Ozone is the main absorber standing between solar UVB and the ground, so where the column thins, more ultraviolet arrives.<\/figcaption>\n<\/figure>\n\n<h2>Why Ultraviolet Does Things Visible Light Cannot<\/h2>\n\n<p>The effects that matter have a threshold rather than a slope: below a certain energy per photon nothing happens at all, no matter how bright the source, and ultraviolet photons clear thresholds that visible photons cannot reach.<\/p>\n\n<p>Metals make the cleanest demonstration, and this site already publishes the numbers it needs. Prising an electron out of a metal surface costs at least that surface&#8217;s work function, and a photon either brings that much on its own or the electron stays put. Four work functions, four threshold wavelengths, calculated from the same 1239.842:<\/p>\n\n<div class=\"pf-table-scroll\" style=\"display:block;width:100%;max-width:100%;overflow-x:auto;-webkit-overflow-scrolling:touch;margin:1.5em 0;\">\n<table style=\"width:100%;border-collapse:collapse;word-break:break-word;\">\n<thead>\n<tr><th style=\"text-align:left;padding:8px 10px;border-bottom:2px solid #C8932A;font-weight:700;white-space:nowrap;\">Metal<\/th><th style=\"text-align:left;padding:8px 10px;border-bottom:2px solid #C8932A;font-weight:700;white-space:nowrap;\">Work function (eV)<\/th><th style=\"text-align:left;padding:8px 10px;border-bottom:2px solid #C8932A;font-weight:700;white-space:nowrap;\">Threshold wavelength (nm)<\/th><th style=\"text-align:left;padding:8px 10px;border-bottom:2px solid #C8932A;font-weight:700;white-space:nowrap;\">Band that threshold falls in<\/th><\/tr>\n<\/thead>\n<tbody>\n<tr><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">Caesium (Cs)<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">2.1<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">590.40<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">Not UV \u2014 orange light<\/td><\/tr>\n<tr><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">Sodium (Na)<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">2.3<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">539.06<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">Not UV \u2014 green light<\/td><\/tr>\n<tr><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">Zinc (Zn)<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">4.3<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">288.34<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">UVB<\/td><\/tr>\n<tr><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">Copper (Cu)<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">4.7<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">263.80<\/td><td style=\"padding:8px 10px;border-bottom:1px solid #D9CFB8;\">UVC<\/td><\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n\n<p>Now set the most energetic visible photon there is against that column. At 400 nm it carries 3.0996 eV. Caesium at 2.1 eV and sodium at 2.3 eV sit below that, so ordinary visible light frees electrons from both of them.<\/p>\n\n<p>Zinc at 4.3 eV and copper at 4.7 eV sit above it. No visible photon \u2014 no colour, no lamp, no brightness, ever \u2014 will free a single electron from either. Zinc needs 288.34 nm or shorter, which is UVB; copper needs 263.80 nm or shorter, which is UVC.<\/p>\n\n<figure style=\"margin:32px auto;max-width:720px;text-align:center;\">\n  <img src=\"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-content\/uploads\/2026\/09\/ultraviolet-radiation-diagram-02-768x495.jpg\" srcset=\"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-content\/uploads\/2026\/09\/ultraviolet-radiation-diagram-02-768x495.jpg 768w, https:\/\/physicsfundamentalsinfo.com\/blog\/wp-content\/uploads\/2026\/09\/ultraviolet-radiation-diagram-02.jpg 1400w\" sizes=\"auto, (max-width: 760px) 100vw, 720px\" width=\"1400\" height=\"902\" alt=\"Photon energy plotted against wavelength from 100 to 700 nanometres, both axes linear. The gold curve is energy equals 1239.842 divided by the wavelength in nanometres, so it falls steeply from 12.3984 electronvolts at 100 nm to 1.7712 electronvolts at 700 nm and is visibly not a straight line. The ultraviolet part of the range, 100 to 400 nm, is shaded and a dashed vertical rule stands at 400 nm where ultraviolet ends and violet light begins. Four horizontal dashed rules mark the work functions of four metals: copper at 4.7, zinc at 4.3, sodium at 2.3 and caesium at 2.1 electronvolts. Where each rule meets the curve a wine dot marks that metal's threshold wavelength, and a legend on the right lists them: copper 263.80 nm inside UVC, zinc 288.34 nm inside UVB, sodium 539.06 nm in green light and caesium 590.40 nm in orange light. A note beneath states that both axes are linear and that the crossings are the thresholds themselves rather than an illustration of them.\" loading=\"lazy\" decoding=\"async\" style=\"width:100%;height:auto;border-radius:4px;\">\n  <figcaption style=\"font-size:13px;color:#1F2E47;font-style:italic;margin-top:8px;\">Photon energy against wavelength on two linear axes. Because energy goes as one over wavelength the curve is not a straight line, and where it crosses each horizontal work function is that metal&#8217;s threshold \u2014 so the diagram computes the payoff rather than illustrating it.<\/figcaption>\n<\/figure>\n\n<p>The surprise is in the top of the table rather than the bottom. Caesium lets go at 590.40 nm and sodium at 539.06 nm, both of them comfortably inside visible light, so the photoelectric effect is not an ultraviolet phenomenon in general. It becomes one the moment the metal is an ordinary one, which is why the classic experiment is taught with a UV lamp; the experiment itself belongs to our <a href=\"https:\/\/physicsfundamentalsinfo.com\/blog\/modern-physics\/photoelectric-effect\/\">photoelectric effect<\/a> guide.<\/p>\n\n<p>That is the honest version of &#8220;ultraviolet is more damaging&#8221;. Not stronger, not hotter, not more abundant \u2014 simply above a bar that visible light never gets over.<\/p>\n\n<p>Chemical bonds work the same way. Ultraviolet photons carry enough energy to break many of them where visible photons generally do not, which is why sunlight yellows plastic and perishes rubber while a bright reading lamp leaves both alone. WHO attributes delayed tanning, burning, skin ageing and a significant contribution to skin cancer to UVB specifically.<\/p>\n\n<h2>Where Ultraviolet Radiation Turns Up in Real Life<\/h2>\n\n<p>Five places, and the wavelength matters in every one of them.<\/p>\n\n<h3>Sunlight on skin<\/h3>\n\n<p>Roughly nineteen parts in twenty of the ultraviolet reaching you outdoors is UVA, on WHO&#8217;s figure of approximately 95 per cent. WHO describes UVB as unable to penetrate beyond the superficial skin layers while being very biologically active there, and UVA as reaching the deeper layers and producing the immediate tanning effect.<\/p>\n\n<h3>Black lights and fluorescence<\/h3>\n\n<p>A black light emits at 365 nm, well inside UVA, and what you actually see is never the ultraviolet. Detergent residues, tonic water, scorpions and the security threads in a banknote all absorb those photons and re-emit the energy at longer, visible wavelengths. The glow is the object&#8217;s answer, not the lamp&#8217;s output.<\/p>\n\n<h3>Germicidal lamps<\/h3>\n\n<p>A low-pressure mercury tube emits strongly at 254 nm, deep in UVC, and 254 nm photons carry 4.8813 eV \u2014 enough to wreck the chemistry that a micro-organism needs in order to copy itself. Those lamps also explain why UVC is handled so carefully: it is the one band sunlight at ground level never delivers, so nobody has any everyday experience of it to calibrate against.<\/p>\n\n<h3>Ultraviolet astronomy<\/h3>\n\n<p>The hottest stars radiate most strongly at wavelengths the atmosphere refuses to pass, which is why ultraviolet astronomy is done from orbit rather than from a mountain top. A telescope on the ground is looking through the same filter that protects the biosphere.<\/p>\n\n<h3>Checking documents and materials<\/h3>\n\n<p>Passports, banknotes and event wristbands carry inks that are invisible under room lighting and obvious under 365 nm. Forensic and conservation work uses the same trick, because many organic residues fluoresce at wavelengths their surroundings do not.<\/p>\n\n<h2>Common Misconceptions About Ultraviolet Radiation<\/h2>\n\n<h3>&#8220;Ultraviolet is ionising radiation&#8221;<\/h3>\n\n<p>Not at the bar that phrase is usually set against. Stripping the electron from a hydrogen atom takes 13.6 eV, which is a photon at 91.16 nm \u2014 shorter than the 100 nm point where ultraviolet even begins. At the 100 nm edge of the range, where ultraviolet is at its most energetic, a photon carries 12.3984 eV: 91.16 per cent of the way there.<\/p>\n\n<p>Be careful with the reverse claim too. Some molecules give up an electron more easily than a hydrogen atom does, so &#8220;ultraviolet never ionises anything&#8221; would be overstating it in the other direction. What is safe to say is that UV sits below the threshold the term is normally defined against, and that its damage is done by breaking bonds. Radiation that ionises reliably starts with X-rays and <a href=\"https:\/\/physicsfundamentalsinfo.com\/blog\/nuclear-physics\/gamma-rays-properties-uses\/\">gamma rays<\/a>.<\/p>\n\n<h3>&#8220;UVC is what burns you at the beach&#8221;<\/h3>\n\n<p>No UVC arrives at the beach. WHO is unambiguous that it is completely filtered by the atmosphere and does not reach the Earth&#8217;s surface, and burning is UVB&#8217;s work. The only UVC anyone meets is made by a lamp.<\/p>\n\n<h3>&#8220;Ultraviolet is just stronger light&#8221;<\/h3>\n\n<p>Strength, in the everyday sense, means photons per second. The threshold cares about energy per photon, and the two are independent. Flood a room with green light at 550 nm and 2.2543 eV and not one electron leaves a zinc surface; a feeble UVC source at 254 nm frees them at once.<\/p>\n\n<h3>&#8220;Ultraviolet is the hot part of sunlight&#8221;<\/h3>\n\n<p>The warmth on your face outdoors is mostly infrared, the band on the long-wavelength side of visible. Ultraviolet is the part you cannot feel arriving at all, which is precisely what makes it worth understanding: there is no sensation to tell you when you have had enough.<\/p>\n\n<h2>Where the Simple Picture Breaks Down<\/h2>\n\n<p>Everything above is accurate and none of it is the whole story. Four places are worth flagging before anyone leans on this page too hard.<\/p>\n\n<p><strong>The band names are labels.<\/strong> A source at 316 nm and one at 314 nm behave almost identically, and they are given different band names. Anything that seems to change abruptly at 280 or 315 nm is an artefact of how the categories were drawn.<\/p>\n\n<p><strong>&#8220;Filtered&#8221; is not a switch.<\/strong> Real atmospheric transmission is a smooth function of wavelength that shifts with the ozone column above you, your altitude and how high the sun is sitting. WHO&#8217;s three verdicts summarise that; they do not calculate it. Nothing here predicts how much ultraviolet arrives at a given place and time, and no dose, exposure or UV index figure appears anywhere on this page.<\/p>\n\n<p><strong>A work function belongs to a surface.<\/strong> The 4.3 eV quoted for zinc is a textbook figure for a clean face of the metal, and real surfaces oxidise, adsorb gas and get handled. Move the work function and the threshold wavelength moves with it, so 288.34 nm is the right answer to the calculation rather than a property you could rely on in a laboratory.<\/p>\n\n<p><strong>One photon, one event.<\/strong> A threshold says whether a single photon can do a job, never how often the job gets done. Damage depends on how many photons arrive as well as on what each one carries, and that is where dose lives \u2014 a different quantity, deliberately absent from this page.<\/p>\n\n<h2>Worked Problems<\/h2>\n\n<div class=\"pf-problem\"><div class=\"pf-problem-num\">Problem 1<\/div><div class=\"pf-problem-question\">A low-pressure mercury germicidal lamp emits at 254 nm. Find the energy of one of its photons in electronvolts and in joules.<\/div><details><summary>Show Solution<\/summary><div class=\"pf-problem-solution\">\n\n<strong>Solution:<\/strong>\n\nStep 1: In the convenient units, the photon energy in electronvolts is 1239.842 divided by the wavelength in nanometres, because 1239.842 eV\u00b7nm is h\u00b7c divided by the elementary charge.\n\nStep 2: 1239.842 \/ 254 = 4.881268 eV, which is 4.8813 eV to four decimal places.\n\nStep 3: Convert to joules by multiplying by the charge on an electron: 4.881268 \u00d7 1.602176634 \u00d7 10<sup>\u221219<\/sup> = 7.8207 \u00d7 10<sup>\u221219<\/sup> J to five significant figures.\n\n<strong>Answer: 4.8813 eV, or 7.8207 \u00d7 10<sup>\u221219<\/sup> J<\/strong>\n\nBoth numbers describe one photon. A lamp emitting a watt at this wavelength is sending out more than 10<sup>18<\/sup> of them a second.\n\n<\/div><\/details><\/div>\n\n<div class=\"pf-problem\"><div class=\"pf-problem-num\">Problem 2<\/div><div class=\"pf-problem-question\">Sunburn is caused mostly by wavelengths around 300 nm. Which UV band is 300 nm in, and how much energy does one of those photons carry?<\/div><details><summary>Show Solution<\/summary><div class=\"pf-problem-solution\">\n\n<strong>Solution:<\/strong>\n\nStep 1: Classify first. The bands are UVC from 100 to 280 nm, UVB from 280 to 315 nm and UVA from 315 to 400 nm, with each band owning its short edge. 300 nm falls between 280 and 315, so it is UVB.\n\nStep 2: Now the energy. 1239.842 \/ 300 = 4.132807 eV, which is 4.1328 eV to four decimal places.\n\nStep 3: Check it against the band. UVB runs from 3.9360 eV at its 315 nm edge to 4.4280 eV at its 280 nm edge, and 4.1328 eV sits inside that interval, so the two answers agree.\n\n<strong>Answer: 300 nm is UVB, and each photon carries 4.1328 eV<\/strong>\n\n<\/div><\/details><\/div>\n\n<div class=\"pf-problem\"><div class=\"pf-problem-num\">Problem 3<\/div><div class=\"pf-problem-question\">A detector responds to photons of 4.00 eV and above. What is the longest wavelength it can see, and which band is that?<\/div><details><summary>Show Solution<\/summary><div class=\"pf-problem-solution\">\n\n<strong>Solution:<\/strong>\n\nStep 1: Longest wavelength means lowest energy, so the threshold wavelength is the one whose photon carries exactly 4.00 eV. Rearranging the same relation gives the wavelength in nanometres as 1239.842 divided by the energy in electronvolts.\n\nStep 2: 1239.842 \/ 4.00 = 309.9605 nm, which is 309.96 nm to two decimal places.\n\nStep 3: Classify it. 309.96 nm lies between 280 and 315 nm, so it is UVB. Check the arithmetic with the invariant: 4.00 \u00d7 309.9605 = 1239.842, as it must be.\n\n<strong>Answer: 309.96 nm, which is UVB<\/strong>\n\n<\/div><\/details><\/div>\n\n<div class=\"pf-problem\"><div class=\"pf-problem-num\">Problem 4<\/div><div class=\"pf-problem-question\">Photochemists quote bond and photon energies in kilojoules per mole. Express the energy of a 315 nm photon in kJ\/mol.<\/div><details><summary>Show Solution<\/summary><div class=\"pf-problem-solution\">\n\n<strong>Solution:<\/strong>\n\nStep 1: Work out the energy of one photon first. 1239.842 \/ 315 = 3.9360 eV to four decimal places.\n\nStep 2: Scale one photon up to a mole. One electronvolt per particle is 96.48533212 kJ per mole, which is the elementary charge multiplied by the Avogadro constant and divided by a thousand.\n\nStep 3: 3.9360 \u00d7 96.48533212 = 379.7663 kJ\/mol, which is 379.8 kJ\/mol to four significant figures.\n\n<strong>Answer: 379.8 kJ\/mol<\/strong>\n\nThat is the UVA side of the UVA\/UVB boundary, and it lands in the same range as the strength of many single covalent bonds \u2014 which is why photochemistry happens at these wavelengths rather than in the visible.\n\n<\/div><\/details><\/div>\n\n<div class=\"pf-problem\"><div class=\"pf-problem-num\">Problem 5<\/div><div class=\"pf-problem-question\">Zinc has a work function of 4.3 eV. Find the longest wavelength that can free an electron from it, say which band that is, and show that no visible photon can do the job.<\/div><details><summary>Show Solution<\/summary><div class=\"pf-problem-solution\">\n\n<strong>Solution:<\/strong>\n\nStep 1: An electron escapes only if one photon brings at least the work function, so the threshold photon carries exactly 4.3 eV and the threshold wavelength is 1239.842 divided by 4.3.\n\nStep 2: 1239.842 \/ 4.3 = 288.3353 nm, which is 288.34 nm to two decimal places. That lies between 280 and 315 nm, so zinc&#8217;s threshold is inside UVB.\n\nStep 3: Test visible light. The shortest visible wavelength is about 400 nm, and 1239.842 \/ 400 = 3.0996 eV. The shortfall is 4.3 \u2212 3.0996 = 1.2004 eV, so even the most energetic visible photon falls well short.\n\n<strong>Answer: 288.34 nm, inside UVB. No visible photon reaches 4.3 eV, so visible light of any brightness frees nothing from zinc<\/strong>\n\n<\/div><\/details><\/div>\n\n<div class=\"pf-problem\"><div class=\"pf-problem-num\">Problem 6<\/div><div class=\"pf-problem-question\">Copper has a work function of 4.7 eV. Find its threshold wavelength, and find the maximum kinetic energy an electron leaves with when copper and zinc are each lit by the 254 nm germicidal line.<\/div><details><summary>Show Solution<\/summary><div class=\"pf-problem-solution\">\n\n<strong>Solution:<\/strong>\n\nStep 1: Threshold first. 1239.842 \/ 4.7 = 263.7962 nm, which is 263.80 nm to two decimal places. That is below 280 nm, so copper&#8217;s threshold sits inside UVC \u2014 a band sunlight never delivers to the ground.\n\nStep 2: Whatever energy the photon brings beyond the work function is left to the electron as kinetic energy. From problem 1, a 254 nm photon carries 4.8813 eV.\n\nStep 3: For copper, 4.8813 \u2212 4.7 = 0.1813 eV. For zinc, 4.8813 \u2212 4.3 = 0.5813 eV.\n\n<strong>Answer: copper&#8217;s threshold is 263.80 nm (UVC); at 254 nm an electron leaves copper with at most 0.1813 eV and zinc with at most 0.5813 eV<\/strong>\n\nSame lamp, same photon, and the electrons come off zinc with 0.5813 \/ 0.1813 = 3.21 times the energy. The difference is entirely the metal&#8217;s.\n\n<\/div><\/details><\/div>\n\n<div class=\"pf-problem\"><div class=\"pf-problem-num\">Problem 7<\/div><div class=\"pf-problem-question\">Ionising a hydrogen atom takes 13.6 eV. Find the wavelength of a photon carrying that energy, and work out how close the most energetic ultraviolet photon gets to it.<\/div><details><summary>Show Solution<\/summary><div class=\"pf-problem-solution\">\n\n<strong>Solution:<\/strong>\n\nStep 1: Turn the energy into a wavelength the same way as before: 1239.842 divided by the energy in electronvolts.\n\nStep 2: 1239.842 \/ 13.6 = 91.1649 nm, which is 91.16 nm to two decimal places. That is shorter than 100 nm, so a photon able to ionise hydrogen is not ultraviolet at all \u2014 it is past the short end of the range.\n\nStep 3: Compare the two energies directly. The most energetic ultraviolet photon sits at 100 nm and carries 12.3984 eV, and 12.3984 \/ 13.6 = 0.911647, which is 91.16 per cent.\n\n<strong>Answer: 91.16 nm, which is outside ultraviolet. The most energetic UV photon reaches 91.16 per cent of hydrogen&#8217;s ionisation energy and stops there<\/strong>\n\nIt is no coincidence that 91.16 turns up twice. The ionisation wavelength is 91.16 per cent of the 100 nm edge, and comparing the two energies gives the same figure with the roles of the two photons swapped, because both divisions run through the same constant. Hydrogen&#8217;s 13.6 eV comes from the <a href=\"https:\/\/physicsfundamentalsinfo.com\/blog\/modern-physics\/bohr-model\/\">Bohr model<\/a>.\n\n<\/div><\/details><\/div>\n\n<h2>Frequently Asked Questions<\/h2>\n\n<details class=\"pf-faq-item\"><summary>What is the wavelength range of ultraviolet radiation?<\/summary><div class=\"pf-faq-item-answer\">\n\nUltraviolet radiation runs from 100 to 400 nm. That range sits between X-rays at the short end and violet light at the long end, and it is divided into three bands: UVC from 100 to 280 nm, UVB from 280 to 315 nm and UVA from 315 to 400 nm. Expressed as photon energy, the same range is 3.0996 to 12.3984 eV.\n\n<\/div><\/details>\n\n<details class=\"pf-faq-item\"><summary>What are UVA, UVB and UVC?<\/summary><div class=\"pf-faq-item-answer\">\n\nUVA, UVB and UVC are the three conventional slices of the 100 to 400 nm range, with the World Health Organization drawing the lines at 315 nm and 280 nm. The names track how far each band gets through the atmosphere and how it behaves in tissue. The boundaries themselves are agreed values rather than physical edges, so nothing measurable changes as a wave crosses one.\n\n<\/div><\/details>\n\n<details class=\"pf-faq-item\"><summary>Which types of UV reach the ground?<\/summary><div class=\"pf-faq-item-answer\">\n\nUVA does, UVB partly does and UVC does not. WHO reports that UVA makes up approximately 95 per cent of the ultraviolet arriving at the Earth&#8217;s surface, that most solar UVB is stopped on the way down, and that UVC is removed completely. The four absorbers named are ozone, water vapour, oxygen and carbon dioxide in the air above you.\n\n<\/div><\/details>\n\n<details class=\"pf-faq-item\"><summary>Is ultraviolet radiation a form of ionising radiation?<\/summary><div class=\"pf-faq-item-answer\">\n\nNot at the energies inside the band. Ionising a hydrogen atom costs 13.6 eV, which is a photon at 91.16 nm, shorter than where ultraviolet even begins at 100 nm. The most energetic UV photon carries 12.3984 eV, reaching 91.16 per cent of that bar. Ultraviolet does its damage by breaking chemical bonds, a far lower requirement, and reliable ionisation starts with X-rays.\n\n<\/div><\/details>\n\n<details class=\"pf-faq-item\"><summary>Why can the eye not see ultraviolet light?<\/summary><div class=\"pf-faq-item-answer\">\n\nHuman photoreceptors stop responding at about 400 nm, so an ultraviolet photon produces no signal to see. That cut-off is where the name comes from: ultra-violet is what lies past the violet end of vision. A black light looks faintly purple and makes objects glow, but the glow is visible light the object re-emits after absorbing 365 nm ultraviolet.\n\n<\/div><\/details>\n\n<details class=\"pf-faq-item\"><summary>Why does ultraviolet light damage skin and plastics when visible light does not?<\/summary><div class=\"pf-faq-item-answer\">\n\nBecause the damage depends on the energy of each individual photon rather than on how many arrive. Breaking a chemical bond or freeing an electron needs a minimum photon energy, and visible photons top out at 3.0996 eV, at 400 nm. Ultraviolet photons clear thresholds that visible photons fall short of. Brightness changes how often that happens, never whether it can happen at all.\n\n<\/div><\/details>\n","protected":false},"excerpt":{"rendered":"<p>Ultraviolet radiation is the 100 to 400 nm region of the electromagnetic spectrum, split by convention into UVA, UVB and UVC. This page gives the three band boundaries and where they come from, the energy every ultraviolet photon carries in eV, joules and kJ\/mol, which bands the atmosphere lets through and why, and the work-function threshold that explains why ultraviolet damages what visible light leaves alone. Seven worked problems, two original diagrams, an interactive lab and a calculator.<\/p>\n","protected":false},"author":1,"featured_media":2118,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[4],"tags":[],"class_list":["post-2115","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-waves"],"_links":{"self":[{"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/posts\/2115","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/comments?post=2115"}],"version-history":[{"count":4,"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/posts\/2115\/revisions"}],"predecessor-version":[{"id":2139,"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/posts\/2115\/revisions\/2139"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/media\/2118"}],"wp:attachment":[{"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/media?parent=2115"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/categories?post=2115"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/tags?post=2115"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}