{"id":476,"date":"2026-07-13T21:08:10","date_gmt":"2026-07-13T21:08:10","guid":{"rendered":"https:\/\/physicsfundamentalsinfo.com\/blog\/?p=476"},"modified":"2026-07-13T23:30:12","modified_gmt":"2026-07-13T23:30:12","slug":"dispersion-of-light","status":"publish","type":"post","link":"https:\/\/physicsfundamentalsinfo.com\/blog\/waves\/dispersion-of-light\/","title":{"rendered":"Dispersion of Light and Prisms"},"content":{"rendered":"\n<div class=\"pf-citation\"><div class=\"eyebrow\">Definition<\/div><p>\n\nDispersion of light is the splitting of white light into its constituent colours when it passes through a transparent medium such as a glass prism, because the refractive index \u2014 and therefore the speed and bending of light \u2014 depends on its wavelength. Shorter wavelengths (violet) slow and bend the most; longer wavelengths (red) bend the least.\n\n<\/p><\/div>\n\n<p>Look at a rainbow arcing over wet fields, or the buried flash of colour deep inside a cut diamond, and you are watching one quiet rule of physics at work. White light is not a single thing \u2014 it is a bundle of colours travelling together, and the right piece of glass or water can pull them apart.<\/p>\n\n<p>That unbundling is dispersion. It is why a cheap glass prism throws a spectrum across your wall, why the sky answers a rainstorm with colour, and why the lens in a phone camera has to fight faint coloured fringes. Once you understand the mechanism, you start to see it everywhere.<\/p>\n\n<h2>What Is Dispersion of Light?<\/h2>\n\n<p>Dispersion of light is the separation of white light into its component colours as it passes through a medium, caused by the refractive index of that medium changing with wavelength. Because each colour bends by a slightly different amount, they emerge fanned out into a spectrum instead of staying blended.<\/p>\n\n<p>Isaac Newton settled the question in the 1660s. Passing sunlight through a prism, he saw the familiar band of red, orange, yellow, green, blue and violet. The clever part came next: a second prism recombined the colours back into white light. That proved the prism was not <em>adding<\/em> anything \u2014 the colours were inside the white light all along, waiting to be spread out.<\/p>\n\n<p>The visible spectrum runs from roughly 400 nm (violet) to 700 nm (red). Each of those wavelengths corresponds to a colour your eye reads, and \u2014 crucially \u2014 to a slightly different refractive index inside glass. Hold that one idea and the rest of dispersion follows.<\/p>\n\n<svg role=\"img\" aria-label=\"White light entering a triangular glass prism and dispersing into a spectrum from red to violet, with violet deviated more than red\" viewBox=\"0 0 700 420\" xmlns=\"http:\/\/www.w3.org\/2000\/svg\"><rect x=\"0\" y=\"0\" width=\"700\" height=\"420\" rx=\"10\" fill=\"#F5F2EA\"><\/rect><polygon points=\"350,72 252,300 448,300\" fill=\"#142139\" fill-opacity=\"0.9\" stroke=\"#C8932A\" stroke-width=\"3\" stroke-linejoin=\"round\"><\/polygon><text x=\"350\" y=\"252\" font-family=\"Manrope, Arial, sans-serif\" font-size=\"15\" fill=\"#FAF6EE\" text-anchor=\"middle\" font-weight=\"600\">Glass prism<\/text><text x=\"350\" y=\"100\" font-family=\"Manrope, Arial, sans-serif\" font-size=\"13\" fill=\"#C8932A\" text-anchor=\"middle\">A<\/text><line x1=\"60\" y1=\"182\" x2=\"299\" y2=\"182\" stroke=\"#0A1628\" stroke-width=\"7\"><\/line><line x1=\"60\" y1=\"182\" x2=\"299\" y2=\"182\" stroke=\"#FAF6EE\" stroke-width=\"3.5\"><\/line><text x=\"150\" y=\"170\" font-family=\"Manrope, Arial, sans-serif\" font-size=\"14\" fill=\"#0A1628\" text-anchor=\"middle\" font-weight=\"600\">White light<\/text><line x1=\"299\" y1=\"182\" x2=\"404\" y2=\"240\" stroke=\"#FAF6EE\" stroke-width=\"3.5\"><\/line><line x1=\"404\" y1=\"240\" x2=\"590\" y2=\"250\" stroke=\"#D6352B\" stroke-width=\"3\"><\/line><line x1=\"404\" y1=\"240\" x2=\"590\" y2=\"263\" stroke=\"#E07B27\" stroke-width=\"3\"><\/line><line x1=\"404\" y1=\"240\" x2=\"590\" y2=\"276\" stroke=\"#D9B62C\" stroke-width=\"3\"><\/line><line x1=\"404\" y1=\"240\" x2=\"590\" y2=\"289\" stroke=\"#3E9E5B\" stroke-width=\"3\"><\/line><line x1=\"404\" y1=\"240\" x2=\"590\" y2=\"302\" stroke=\"#3A6EA5\" stroke-width=\"3\"><\/line><line x1=\"404\" y1=\"240\" x2=\"590\" y2=\"315\" stroke=\"#7A4FA5\" stroke-width=\"3\"><\/line><text x=\"598\" y=\"254\" font-family=\"Manrope, Arial, sans-serif\" font-size=\"12\" fill=\"#B02B22\">Red<\/text><text x=\"598\" y=\"280\" font-family=\"Manrope, Arial, sans-serif\" font-size=\"12\" fill=\"#8A6A17\">Yellow<\/text><text x=\"598\" y=\"306\" font-family=\"Manrope, Arial, sans-serif\" font-size=\"12\" fill=\"#2F5A86\">Blue<\/text><text x=\"598\" y=\"319\" font-family=\"Manrope, Arial, sans-serif\" font-size=\"12\" fill=\"#5F3F86\">Violet<\/text><\/svg>\n\n<p style=\"text-align:center;font-size:13px;color:#1F2E47;font-style:italic;\">White light entering a prism is bent twice. Violet is deviated most and red least, so the beam leaves fanned into a spectrum.<\/p>\n\n<h2>The Formulas Behind Dispersion of Light<\/h2>\n\n<p>Dispersion has no single master equation \u2014 it emerges from the law of refraction fed by one fact: the refractive index <strong>n<\/strong> is a function of wavelength. Start with Snell&#8217;s law, which governs how any ray bends at a boundary.<\/p>\n\n<div class=\"pf-formula\">n<sub>1<\/sub> sin \u03b8<sub>1<\/sub> = n<sub>2<\/sub> sin \u03b8<sub>2<\/sub><\/div>\n\n<ul>\n<li><strong>n<sub>1<\/sub>, n<sub>2<\/sub><\/strong> \u2014 refractive indices of the first and second media (dimensionless)<\/li>\n<li><strong>\u03b8<sub>1<\/sub><\/strong> \u2014 angle of incidence, measured from the normal (radians in SI; usually quoted in degrees)<\/li>\n<li><strong>\u03b8<sub>2<\/sub><\/strong> \u2014 angle of refraction, from the normal (radians or degrees)<\/li>\n<\/ul>\n\n<p>Because n<sub>2<\/sub> is slightly different for each colour, \u03b8<sub>2<\/sub> comes out different for each colour. That single line contains the whole of dispersion in miniature. You can test any pair of media with our <a href=\"https:\/\/physicsfundamentalsinfo.com\/calculators\/snells-law\">Snell&#8217;s Law Calculator<\/a>.<\/p>\n\n<p>Why does n differ between colours? It comes back to speed.<\/p>\n\n<div class=\"pf-formula\">n = c \/ v<\/div>\n\n<ul>\n<li><strong>n<\/strong> \u2014 refractive index of the medium (dimensionless)<\/li>\n<li><strong>c<\/strong> \u2014 speed of light in vacuum, 299,792,458 m\/s<\/li>\n<li><strong>v<\/strong> \u2014 speed of light in the medium (m\/s)<\/li>\n<\/ul>\n\n<p>A larger n means light crawls more slowly through the material. Violet light has the highest n in glass, so it is the slowest colour inside a prism \u2014 and, by Snell&#8217;s law, the most sharply bent.<\/p>\n\n<p>The wavelength dependence itself is captured well by Cauchy&#8217;s empirical relation, which describes <em>normal<\/em> dispersion across the visible range.<\/p>\n\n<div class=\"pf-formula\">n(\u03bb) = A + B \/ \u03bb<sup>2<\/sup><\/div>\n\n<ul>\n<li><strong>n(\u03bb)<\/strong> \u2014 refractive index at wavelength \u03bb (dimensionless)<\/li>\n<li><strong>A, B<\/strong> \u2014 constants unique to the material (A is dimensionless; B has units of length<sup>2<\/sup>, usually \u00b5m<sup>2<\/sup>)<\/li>\n<li><strong>\u03bb<\/strong> \u2014 wavelength of the light (metres in SI; normally quoted in nm or \u00b5m)<\/li>\n<\/ul>\n\n<p>As \u03bb falls toward the violet end, the B\/\u03bb<sup>2<\/sup> term grows, so n rises. That is the mathematical fingerprint of &#8220;violet bends more than red.&#8221;<\/p>\n\n<p>For a whole prism, the practical relationship is the <strong>angle of minimum deviation<\/strong> \u2014 the workhorse of the optics bench, and the &#8220;prism rule&#8221; that lets you measure a glass&#8217;s refractive index directly.<\/p>\n\n<div class=\"pf-formula\">n = sin[(A + \u03b4<sub>min<\/sub>) \/ 2] \/ sin(A \/ 2)<\/div>\n\n<ul>\n<li><strong>n<\/strong> \u2014 refractive index of the prism for that colour (dimensionless)<\/li>\n<li><strong>A<\/strong> \u2014 the refracting (apex) angle of the prism (degrees or radians)<\/li>\n<li><strong>\u03b4<sub>min<\/sub><\/strong> \u2014 angle of minimum deviation for that colour (degrees or radians)<\/li>\n<\/ul>\n\n<p>Measure the smallest deviation a prism produces for each colour and you can read off that colour&#8217;s refractive index. Since \u03b4<sub>min<\/sub> is larger for violet, this returns a larger n for violet than for red \u2014 the numbers agree with the physics.<\/p>\n\n<p>Two more quantities matter for <em>how wide<\/em> the spectrum spreads. For a thin prism, one colour is deviated by \u03b4 = (n &#8211; 1)A, so the <strong>angular dispersion<\/strong> between violet and red is (n<sub>V<\/sub> &#8211; n<sub>R<\/sub>)A. The material&#8217;s <strong>dispersive power<\/strong> \u03c9 = (n<sub>V<\/sub> &#8211; n<sub>R<\/sub>) \/ (n<sub>Y<\/sub> &#8211; 1) then tells you how strongly a glass fans the colours relative to how much it bends light overall.<\/p>\n\n<h2>How Dispersion of Light Works<\/h2>\n\n<p>Dispersion works because light of different wavelengths travels at different speeds inside a medium, and speed controls the amount of bending. Everything else is the story of <em>why<\/em> the speed depends on colour.<\/p>\n\n<p>Light is an electromagnetic wave \u2014 a travelling ripple of electric and magnetic fields. As it enters glass, its oscillating field pushes and pulls on the bound electrons of the atoms, which vibrate and re-radiate their own tiny waves. Those re-radiated waves interfere with the original, and the net result is a wave that advances more slowly than it would in empty space. That slow-down is exactly what the refractive index measures.<\/p>\n\n<p>Here is the key twist. How strongly the electrons respond depends on how close the light&#8217;s frequency is to the material&#8217;s own natural resonances, which for ordinary glass sit in the ultraviolet. Violet light, with its higher frequency, sits closer to those resonances, so it interacts more strongly, is slowed more, and ends up with a higher refractive index. Red light, further from resonance, is slowed less. The colours therefore travel at genuinely different speeds inside the glass.<\/p>\n\n<h3>Why does violet light bend more than red?<\/h3>\n\n<p>Violet bends more than red because most transparent materials have a higher refractive index for shorter wavelengths. A higher index means a slower speed, and Snell&#8217;s law turns that slower speed into a larger deflection angle at the surface. Red, at the long-wavelength end, has the lowest index and bends least \u2014 which is why red always sits on the outer edge of a spectrum and violet on the inner.<\/p>\n\n<p>The size of the effect is small but real. In a typical crown glass the index shifts by only about one part in a hundred across the visible band, yet that is enough to smear white light into a clean spectrum.<\/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>\n<th style=\"border:1px solid #D9CFB8;padding:8px;text-align:left;background:#142139;color:#FAF6EE;\">Colour<\/th>\n<th style=\"border:1px solid #D9CFB8;padding:8px;text-align:left;background:#142139;color:#FAF6EE;\">Approx. wavelength (nm)<\/th>\n<th style=\"border:1px solid #D9CFB8;padding:8px;text-align:left;background:#142139;color:#FAF6EE;\">Refractive index n (typical crown glass)<\/th>\n<\/tr>\n<\/thead>\n<tbody>\n<tr><td style=\"border:1px solid #D9CFB8;padding:8px;\">Red<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">\u2248 660<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">1.513<\/td><\/tr>\n<tr><td style=\"border:1px solid #D9CFB8;padding:8px;\">Yellow<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">\u2248 590<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">1.517<\/td><\/tr>\n<tr><td style=\"border:1px solid #D9CFB8;padding:8px;\">Green<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">\u2248 530<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">1.519<\/td><\/tr>\n<tr><td style=\"border:1px solid #D9CFB8;padding:8px;\">Blue<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">\u2248 490<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">1.522<\/td><\/tr>\n<tr><td style=\"border:1px solid #D9CFB8;padding:8px;\">Violet<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">\u2248 410<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">1.530<\/td><\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n\n<p style=\"font-size:13px;color:#1F2E47;\"><em>Values are approximate for a typical crown glass and vary with composition. The trend \u2014 n rising steadily toward violet \u2014 is the point.<\/em><\/p>\n\n<svg role=\"img\" aria-label=\"Graph of refractive index versus wavelength showing the index falling as wavelength increases from violet to red\" viewBox=\"0 0 700 400\" xmlns=\"http:\/\/www.w3.org\/2000\/svg\"><rect x=\"0\" y=\"0\" width=\"700\" height=\"400\" rx=\"10\" fill=\"#F5F2EA\"><\/rect><line x1=\"95\" y1=\"330\" x2=\"640\" y2=\"330\" stroke=\"#0A1628\" stroke-width=\"2\"><\/line><line x1=\"95\" y1=\"330\" x2=\"95\" y2=\"60\" stroke=\"#0A1628\" stroke-width=\"2\"><\/line><text x=\"367\" y=\"374\" font-family=\"Manrope, Arial, sans-serif\" font-size=\"14\" fill=\"#0A1628\" text-anchor=\"middle\">Wavelength \u03bb (nm)<\/text><text x=\"42\" y=\"195\" font-family=\"Manrope, Arial, sans-serif\" font-size=\"14\" fill=\"#0A1628\" text-anchor=\"middle\" transform=\"rotate(-90 42 195)\">Refractive index n<\/text><line x1=\"150\" y1=\"330\" x2=\"150\" y2=\"336\" stroke=\"#0A1628\" stroke-width=\"2\"><\/line><text x=\"150\" y=\"352\" font-family=\"Manrope, Arial, sans-serif\" font-size=\"12\" fill=\"#0A1628\" text-anchor=\"middle\">400<\/text><line x1=\"303\" y1=\"330\" x2=\"303\" y2=\"336\" stroke=\"#0A1628\" stroke-width=\"2\"><\/line><text x=\"303\" y=\"352\" font-family=\"Manrope, Arial, sans-serif\" font-size=\"12\" fill=\"#0A1628\" text-anchor=\"middle\">500<\/text><line x1=\"456\" y1=\"330\" x2=\"456\" y2=\"336\" stroke=\"#0A1628\" stroke-width=\"2\"><\/line><text x=\"456\" y=\"352\" font-family=\"Manrope, Arial, sans-serif\" font-size=\"12\" fill=\"#0A1628\" text-anchor=\"middle\">600<\/text><line x1=\"610\" y1=\"330\" x2=\"610\" y2=\"336\" stroke=\"#0A1628\" stroke-width=\"2\"><\/line><text x=\"610\" y=\"352\" font-family=\"Manrope, Arial, sans-serif\" font-size=\"12\" fill=\"#0A1628\" text-anchor=\"middle\">700<\/text><path d=\"M 150 100 C 300 150, 430 250, 610 300\" fill=\"none\" stroke=\"#C8932A\" stroke-width=\"4\"><\/path><circle cx=\"150\" cy=\"100\" r=\"6\" fill=\"#7A4FA5\"><\/circle><text x=\"165\" y=\"98\" font-family=\"Manrope, Arial, sans-serif\" font-size=\"12\" fill=\"#5F3F86\">Violet: larger n<\/text><circle cx=\"610\" cy=\"300\" r=\"6\" fill=\"#D6352B\"><\/circle><text x=\"470\" y=\"298\" font-family=\"Manrope, Arial, sans-serif\" font-size=\"12\" fill=\"#B02B22\">Red: smaller n<\/text><text x=\"367\" y=\"88\" font-family=\"Manrope, Arial, sans-serif\" font-size=\"13\" fill=\"#7A1F2B\" text-anchor=\"middle\" font-weight=\"600\">Normal dispersion: n falls as wavelength rises<\/text><\/svg>\n\n<p style=\"text-align:center;font-size:13px;color:#1F2E47;font-style:italic;\">A dispersion curve for a typical glass. Short wavelengths have the highest index, so they slow and bend the most.<\/p>\n\n<p>A single flat window would refract all the colours and then un-refract them at the parallel far surface, so they leave recombined \u2014 no visible spectrum. A prism is different. Its two faces are tilted relative to each other, so the second refraction <em>adds<\/em> to the first instead of cancelling it. That is why a prism, and not a flat pane, throws a rainbow.<\/p>\n\n<p>One practical detail worth knowing: as you slowly rotate a prism, the total bending of a given colour dips to a minimum when the ray passes symmetrically through the glass. That symmetric geometry is the angle of minimum deviation used in the &#8220;prism rule&#8221; above, and it is where lab measurements are taken.<\/p>\n\n<div class=\"pf-sim-slot\"><div class=\"pf-sim-slot-header\"><span class=\"icon-dot\"><\/span><span class=\"label\">Prism Dispersion Lab<\/span><\/div><div class=\"pf-sim-slot-body\">\n<style>\n.pf-sim-frame{\nwidth:100%;\nborder:none;\nheight:600px\n}\n@media(max-width:760px){\n.pf-sim-frame{\nheight:1000px\n}\n}\n<\/style>\n<iframe src=\"\/labs\/dispersion-of-light.html?embed=1\" class=\"pf-sim-frame\" loading=\"lazy\">\n<\/iframe>\n<\/div><\/div>\n\n<h2>Real-World Examples of Dispersion of Light<\/h2>\n\n<p>Dispersion is not a lab curiosity \u2014 it paints the sky, cuts fire into gemstones, and quietly limits the cameras and telescopes we build. Here are seven places it shows up.<\/p>\n\n<p><strong>Rainbows.<\/strong> Each raindrop acts as a tiny prism-plus-mirror: sunlight refracts on the way in, reflects off the back of the drop, and refracts again on the way out, emerging spread into colours. Because red is bent least and violet most, the primary bow shows red at about a 42\u00b0 angle and violet near 40\u00b0, with red on the outer edge \u2014 exactly as described by <a href=\"https:\/\/scijinks.gov\/rainbow\/\" target=\"_blank\" rel=\"noopener\">NOAA&#8217;s SciJinks<\/a>. A fainter secondary bow, formed by a second internal reflection, appears higher up at around 50\u00b0 with its colours reversed, a geometry laid out by the <a href=\"https:\/\/www.weather.gov\/fgz\/Rainbow\" target=\"_blank\" rel=\"noopener\">US National Weather Service<\/a>.<\/p>\n\n<p><strong>The glass prism.<\/strong> The triangular prism is the textbook icon of dispersion for good reason \u2014 it is the cleanest way to turn a beam of white light into a visible spectrum, and it is exactly what Newton used to prove that colour lives inside white light.<\/p>\n\n<p><strong>Diamond and gemstone &#8220;fire.&#8221;<\/strong> Diamond combines a very high refractive index (about 2.42) with strong dispersion (a spread of 0.044 across the spectrum). Light bends sharply on entry, bounces around inside the cut stone by total internal reflection, and fans into colours on the way out, so a diamond throws flashes of red, blue and green. Moissanite disperses even more strongly (0.104), which is why it can look almost too colourful to a trained eye.<\/p>\n\n<p><strong>Chromatic aberration.<\/strong> A simple lens is a curved piece of glass, so it disperses too \u2014 it focuses blue light slightly closer than red, leaving coloured fringes around edges in cheap binoculars and older cameras. The fix is an achromatic doublet: a low-dispersion crown-glass element cemented to a high-dispersion flint element, engineered so two wavelengths land at the same focus.<\/p>\n\n<p><strong>Spectrometers.<\/strong> Spread starlight or a flame&#8217;s glow with a prism or grating and you get a spectrum crossed by dark or bright lines \u2014 the fingerprints of individual elements. Dispersion is the reason we can measure what distant stars are made of without ever leaving Earth.<\/p>\n\n<p><strong>The green flash.<\/strong> Right as the Sun dips below a clean horizon, the atmosphere disperses its image into faintly overlapping coloured discs. With the blue scattered away, the last visible sliver can briefly flash green \u2014 a rare, genuine piece of atmospheric dispersion.<\/p>\n\n<p><strong>Sundogs and haloes.<\/strong> High, thin cloud full of hexagonal ice crystals turns each crystal into a miniature prism. The result is the 22\u00b0 halo around the Sun or Moon and the bright &#8220;sundogs&#8221; beside it, often tinged red on their sunward edge.<\/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\/07\/Light_dispersion_of_a_mercury-vapor_lamp_with_a_flint_glass_prism_IPNr\u00b00125.jpg\"\n       alt=\"Dispersion of light: white light splitting into a rainbow spectrum through a glass prism\"\n       loading=\"lazy\"\n       style=\"width:100%;height:auto;border-radius:4px;\" \/>\n  <figcaption style=\"font-size:13px;color:#1F2E47;font-style:italic;margin-top:8px;\">A real prism dispersing white light into its component colours.<\/figcaption>\n<\/figure>\n\n<p>Notice what these share: colour spreading from a change in speed. The stronger a material disperses, the wider it fans the spectrum.<\/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>\n<th style=\"border:1px solid #D9CFB8;padding:8px;text-align:left;background:#142139;color:#FAF6EE;\">Medium<\/th>\n<th style=\"border:1px solid #D9CFB8;padding:8px;text-align:left;background:#142139;color:#FAF6EE;\">Refractive index n (\u2248 589 nm)<\/th>\n<th style=\"border:1px solid #D9CFB8;padding:8px;text-align:left;background:#142139;color:#FAF6EE;\">Abbe number V<sub>d<\/sub><\/th>\n<th style=\"border:1px solid #D9CFB8;padding:8px;text-align:left;background:#142139;color:#FAF6EE;\">Dispersion<\/th>\n<\/tr>\n<\/thead>\n<tbody>\n<tr><td style=\"border:1px solid #D9CFB8;padding:8px;\">Air<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">1.0003<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">\u2014<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">Negligible<\/td><\/tr>\n<tr><td style=\"border:1px solid #D9CFB8;padding:8px;\">Water<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">1.333<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">\u2248 55.6<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">Low<\/td><\/tr>\n<tr><td style=\"border:1px solid #D9CFB8;padding:8px;\">Fused quartz<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">1.458<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">\u2248 67.8<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">Very low<\/td><\/tr>\n<tr><td style=\"border:1px solid #D9CFB8;padding:8px;\">Crown glass (BK7)<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">1.5168<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">\u2248 64.2<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">Low<\/td><\/tr>\n<tr><td style=\"border:1px solid #D9CFB8;padding:8px;\">Flint glass (F2)<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">1.620<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">\u2248 36.4<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">High<\/td><\/tr>\n<tr><td style=\"border:1px solid #D9CFB8;padding:8px;\">Dense flint (SF10)<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">1.728<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">\u2248 28.4<\/td><td style=\"border:1px solid #D9CFB8;padding:8px;\">Very high<\/td><\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n\n<p style=\"font-size:13px;color:#1F2E47;\"><em>The Abbe number V<sub>d<\/sub> is the standard optical measure of dispersion \u2014 a <strong>higher<\/strong> number means colours spread <strong>less<\/strong>. Crown glasses sit above about 55; flints fall below.<\/em><\/p>\n\n<h2>Common Misconceptions About Dispersion of Light<\/h2>\n\n<p>A few stubborn misunderstandings trip up almost everyone the first time. Clearing them makes the physics click.<\/p>\n\n<p><strong>&#8220;A prism adds colour to white light.&#8221;<\/strong> It does not. White light already contains every visible colour; the prism only separates what was there. Newton&#8217;s proof was to recombine the spectrum with a second prism and recover plain white light.<\/p>\n\n<p><strong>&#8220;Red light bends the most.&#8221;<\/strong> The opposite is true in ordinary materials. Violet has the highest refractive index, so it is slowed and bent the most, while red bends the least. A common exam slip is to picture red on the inside of the spectrum \u2014 it belongs on the outside.<\/p>\n\n<p><strong>&#8220;All colours travel at the same speed in glass.&#8221;<\/strong> Inside a medium each colour has its own refractive index and therefore its own speed, v = c\/n. Violet is the slowest, red the fastest. They only share a single speed \u2014 c \u2014 when they are back in a vacuum.<\/p>\n\n<p><strong>&#8220;Dispersion and refraction are the same thing.&#8221;<\/strong> Refraction is the bending of light at a boundary; dispersion is the fact that the amount of bending depends on wavelength. A single laser colour refracts without dispersing. You need a spread of wavelengths, plus an index that varies with wavelength, to get dispersion.<\/p>\n\n<h2>How Dispersion Relates to Refraction, Wavelength and the Speed of Light<\/h2>\n\n<p>Dispersion sits at the meeting point of several ideas you may already have met, which is what makes it such a satisfying topic to pin down.<\/p>\n\n<p>It is refraction with a wavelength label attached. Every colour obeys Snell&#8217;s law; dispersion is simply the observation that the law gives a slightly different answer for each wavelength. The reason is speed: light of different colours travels at different rates in a medium, and the <a href=\"https:\/\/physicsfundamentalsinfo.com\/blog\/modern-physics\/speed-of-light\/\">speed of light in a material<\/a> is what the refractive index encodes through n = c\/v.<\/p>\n\n<p>Colour, in turn, is wavelength. Whether a wave reads as red or violet to your eye is set by its wavelength and frequency, linked by the <a href=\"https:\/\/physicsfundamentalsinfo.com\/blog\/waves\/frequency-formula\/\">wave relationship c = f\u03bb<\/a>. Dispersion is only possible because white light is a mixture of many wavelengths rather than one.<\/p>\n\n<p>And it all rests on light being a wave in the first place. Light is a <a href=\"https:\/\/physicsfundamentalsinfo.com\/blog\/waves\/transverse-vs-longitudinal-waves\/\">transverse electromagnetic wave<\/a>, and it is the interaction of that oscillating wave with a material&#8217;s electrons that makes speed depend on frequency. In fact, any wave whose speed depends on wavelength can disperse \u2014 a broader idea you can also see in wave phenomena such as the <a href=\"https:\/\/physicsfundamentalsinfo.com\/blog\/waves\/doppler-effect\/\">Doppler effect<\/a>, where wavelength and frequency again take centre stage.<\/p>\n\n<h2>Worked Problems<\/h2>\n\n<p>Work through these in order \u2014 they build from a one-line speed calculation to a full two-surface prism trace. Carry units and keep to sensible significant figures. Take c \u2248 3.00 \u00d7 10<sup>8<\/sup> m\/s throughout.<\/p>\n\n<div class=\"pf-problem\"><div class=\"pf-problem-num\">Problem 1<\/div><div class=\"pf-problem-question\">A crown glass has refractive index 1.513 for red light and 1.532 for violet light. Find the speed of each colour inside the glass, and say which travels faster.<\/div><details><summary>Show Solution<\/summary><div class=\"pf-problem-solution\">\n\n<p><strong>Solution:<\/strong><\/p>\n<p>Step 1: Use n = c\/v, rearranged to v = c\/n.<\/p>\n<p>Step 2: Red \u2014 v = (3.00 \u00d7 10<sup>8<\/sup> m\/s) \/ 1.513 = 1.98 \u00d7 10<sup>8<\/sup> m\/s.<\/p>\n<p>Step 3: Violet \u2014 v = (3.00 \u00d7 10<sup>8<\/sup> m\/s) \/ 1.532 = 1.96 \u00d7 10<sup>8<\/sup> m\/s.<\/p>\n<p><strong>Answer: red \u2248 1.98 \u00d7 10<sup>8<\/sup> m\/s, violet \u2248 1.96 \u00d7 10<sup>8<\/sup> m\/s. Red travels faster because it has the lower refractive index.<\/strong><\/p>\n\n<\/div><\/details><\/div>\n\n<div class=\"pf-problem\"><div class=\"pf-problem-num\">Problem 2<\/div><div class=\"pf-problem-question\">White light strikes a flat air-glass surface at 40\u00b0 to the normal. Using n = 1.513 (red) and n = 1.532 (violet), find the refraction angle of each colour and the angular separation between them inside the glass.<\/div><details><summary>Show Solution<\/summary><div class=\"pf-problem-solution\">\n\n<p><strong>Solution:<\/strong><\/p>\n<p>Step 1: Apply Snell&#8217;s law, sin \u03b8<sub>2<\/sub> = (n<sub>1<\/sub> sin \u03b8<sub>1<\/sub>) \/ n<sub>2<\/sub>, with n<sub>1<\/sub> = 1.00 and sin 40\u00b0 = 0.6428.<\/p>\n<p>Step 2: Red \u2014 sin \u03b8<sub>2<\/sub> = 0.6428 \/ 1.513 = 0.4249, so \u03b8<sub>2<\/sub> = 25.1\u00b0. Violet \u2014 sin \u03b8<sub>2<\/sub> = 0.6428 \/ 1.532 = 0.4196, so \u03b8<sub>2<\/sub> = 24.8\u00b0.<\/p>\n<p>Step 3: Angular separation = 25.1\u00b0 &#8211; 24.8\u00b0 = 0.3\u00b0.<\/p>\n<p><strong>Answer: red refracts at 25.1\u00b0, violet at 24.8\u00b0, separated by \u2248 0.3\u00b0. Violet sits closer to the normal, confirming it bends more.<\/strong><\/p>\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 thin crown-glass prism has a refracting angle A = 5\u00b0 and refractive index n = 1.52 for yellow light. Find the deviation it produces for yellow light.<\/div><details><summary>Show Solution<\/summary><div class=\"pf-problem-solution\">\n\n<p><strong>Solution:<\/strong><\/p>\n<p>Step 1: For a thin prism, deviation \u03b4 = (n &#8211; 1)A.<\/p>\n<p>Step 2: Substitute \u2014 \u03b4 = (1.52 &#8211; 1) \u00d7 5\u00b0 = 0.52 \u00d7 5\u00b0.<\/p>\n<p>Step 3: \u03b4 = 2.6\u00b0.<\/p>\n<p><strong>Answer: 2.6\u00b0.<\/strong><\/p>\n\n<\/div><\/details><\/div>\n\n<div class=\"pf-problem\"><div class=\"pf-problem-num\">Problem 4<\/div><div class=\"pf-problem-question\">A thin prism has A = 8\u00b0, with n = 1.532 for violet, 1.517 for yellow and 1.513 for red. Find the angular dispersion between violet and red, and the dispersive power of the glass.<\/div><details><summary>Show Solution<\/summary><div class=\"pf-problem-solution\">\n\n<p><strong>Solution:<\/strong><\/p>\n<p>Step 1: Angular dispersion for a thin prism = (n<sub>V<\/sub> &#8211; n<sub>R<\/sub>)A.<\/p>\n<p>Step 2: = (1.532 &#8211; 1.513) \u00d7 8\u00b0 = 0.019 \u00d7 8\u00b0 = 0.152\u00b0 \u2248 0.15\u00b0.<\/p>\n<p>Step 3: Dispersive power \u03c9 = (n<sub>V<\/sub> &#8211; n<sub>R<\/sub>) \/ (n<sub>Y<\/sub> &#8211; 1) = 0.019 \/ (1.517 &#8211; 1) = 0.019 \/ 0.517 = 0.037.<\/p>\n<p><strong>Answer: angular dispersion \u2248 0.15\u00b0; dispersive power \u03c9 \u2248 0.037.<\/strong><\/p>\n\n<\/div><\/details><\/div>\n\n<div class=\"pf-problem\"><div class=\"pf-problem-num\">Problem 5<\/div><div class=\"pf-problem-question\">An equilateral glass prism (A = 60\u00b0) produces a minimum deviation of 39.0\u00b0 for yellow light. Find the refractive index of the glass for yellow light.<\/div><details><summary>Show Solution<\/summary><div class=\"pf-problem-solution\">\n\n<p><strong>Solution:<\/strong><\/p>\n<p>Step 1: Use the prism formula n = sin[(A + \u03b4<sub>min<\/sub>) \/ 2] \/ sin(A \/ 2).<\/p>\n<p>Step 2: (A + \u03b4<sub>min<\/sub>) \/ 2 = (60\u00b0 + 39.0\u00b0) \/ 2 = 49.5\u00b0, and A \/ 2 = 30\u00b0.<\/p>\n<p>Step 3: n = sin 49.5\u00b0 \/ sin 30\u00b0 = 0.7604 \/ 0.5000 = 1.52.<\/p>\n<p><strong>Answer: n \u2248 1.52, a typical value for crown glass.<\/strong><\/p>\n\n<\/div><\/details><\/div>\n\n<div class=\"pf-problem\"><div class=\"pf-problem-num\">Problem 6<\/div><div class=\"pf-problem-question\">Inside a diamond, n = 2.407 for red light and 2.451 for violet light. Find the critical angle for total internal reflection for each colour, and the difference between them.<\/div><details><summary>Show Solution<\/summary><div class=\"pf-problem-solution\">\n\n<p><strong>Solution:<\/strong><\/p>\n<p>Step 1: The critical angle satisfies sin \u03b8<sub>c<\/sub> = 1\/n (diamond to air).<\/p>\n<p>Step 2: Red \u2014 \u03b8<sub>c<\/sub> = arcsin(1 \/ 2.407) = arcsin(0.4155) = 24.6\u00b0. Violet \u2014 \u03b8<sub>c<\/sub> = arcsin(1 \/ 2.451) = arcsin(0.4080) = 24.1\u00b0.<\/p>\n<p>Step 3: Difference = 24.6\u00b0 &#8211; 24.1\u00b0 = 0.5\u00b0.<\/p>\n<p><strong>Answer: red 24.6\u00b0, violet 24.1\u00b0, differing by \u2248 0.5\u00b0. Colours reach total internal reflection at slightly different angles, which helps create a diamond&#8217;s fire.<\/strong><\/p>\n\n<\/div><\/details><\/div>\n\n<div class=\"pf-problem\"><div class=\"pf-problem-num\">Problem 7<\/div><div class=\"pf-problem-question\">White light enters an equilateral prism (A = 60\u00b0) at an angle of incidence of 45\u00b0. Using n = 1.513 (red) and n = 1.532 (violet), find the deviation of each colour and the angular width of the emerging spectrum.<\/div><details><summary>Show Solution<\/summary><div class=\"pf-problem-solution\">\n\n<p><strong>Solution:<\/strong><\/p>\n<p>Step 1: At the first face, sin r<sub>1<\/sub> = sin 45\u00b0 \/ n. Then r<sub>2<\/sub> = A &#8211; r<sub>1<\/sub>, and at the second face sin i<sub>2<\/sub> = n sin r<sub>2<\/sub>. The deviation is \u03b4 = i<sub>1<\/sub> + i<sub>2<\/sub> &#8211; A.<\/p>\n<p>Step 2: Red \u2014 sin r<sub>1<\/sub> = 0.7071 \/ 1.513 = 0.4674, r<sub>1<\/sub> = 27.9\u00b0, r<sub>2<\/sub> = 32.1\u00b0; sin i<sub>2<\/sub> = 1.513 \u00d7 sin 32.1\u00b0 = 0.8048, i<sub>2<\/sub> = 53.6\u00b0; \u03b4<sub>red<\/sub> = 45\u00b0 + 53.6\u00b0 &#8211; 60\u00b0 = 38.6\u00b0.<\/p>\n<p>Step 3: Violet \u2014 sin r<sub>1<\/sub> = 0.7071 \/ 1.532 = 0.4616, r<sub>1<\/sub> = 27.5\u00b0, r<sub>2<\/sub> = 32.5\u00b0; sin i<sub>2<\/sub> = 1.532 \u00d7 sin 32.5\u00b0 = 0.8234, i<sub>2<\/sub> = 55.4\u00b0; \u03b4<sub>violet<\/sub> = 45\u00b0 + 55.4\u00b0 &#8211; 60\u00b0 = 40.4\u00b0.<\/p>\n<p><strong>Answer: red deviates 38.6\u00b0, violet 40.4\u00b0, so the spectrum spans \u2248 1.8\u00b0.<\/strong><\/p>\n\n<\/div><\/details><\/div>\n\n<h2>Frequently Asked Questions<\/h2>\n\n<details class=\"pf-faq-item\"><summary>What is dispersion of light?<\/summary><div class=\"pf-faq-item-answer\">\n\nDispersion of light is the splitting of white light into its component colours as it travels through a medium, because the refractive index of that medium depends on wavelength. Shorter wavelengths (violet) have a higher index, travel more slowly, and bend more than longer wavelengths (red). A glass prism and a raindrop both show it.\n\n<\/div><\/details>\n\n<details class=\"pf-faq-item\"><summary>Why does a prism split white light into colours?<\/summary><div class=\"pf-faq-item-answer\">\n\nA prism splits white light because each colour has a slightly different refractive index in the glass, so each is bent by a different amount at the prism&#8217;s two slanted faces. Violet is bent most and red least, and because the faces are not parallel, the two refractions add together to fan the colours into a visible spectrum.\n\n<\/div><\/details>\n\n<details class=\"pf-faq-item\"><summary>Why does violet light bend more than red light?<\/summary><div class=\"pf-faq-item-answer\">\n\nViolet light bends more than red because the refractive index of most transparent materials is higher for shorter wavelengths. A higher index means violet travels more slowly in the medium and, by Snell&#8217;s law, is deflected through a larger angle. Red, with the longest visible wavelength, has the lowest index and bends the least.\n\n<\/div><\/details>\n\n<details class=\"pf-faq-item\"><summary>Is a rainbow caused by dispersion?<\/summary><div class=\"pf-faq-item-answer\">\n\nYes. A rainbow is caused by dispersion combined with refraction and internal reflection inside raindrops. Sunlight refracts as it enters each drop, reflects off the back, and refracts again on the way out, and because each colour bends by a slightly different amount, the light emerges spread into a spectrum arranged in an arc.\n\n<\/div><\/details>\n\n<details class=\"pf-faq-item\"><summary>Does dispersion of light happen in a vacuum?<\/summary><div class=\"pf-faq-item-answer\">\n\nNo. In a vacuum every wavelength of light travels at exactly the same speed, c, so there is nothing to separate the colours and no dispersion occurs. Dispersion needs a medium \u2014 glass, water, or another transparent material \u2014 in which the speed of light, and therefore the refractive index, changes with wavelength.\n\n<\/div><\/details>\n\n<details class=\"pf-faq-item\"><summary>What is the difference between dispersion and refraction?<\/summary><div class=\"pf-faq-item-answer\">\n\nRefraction is the bending of light as it crosses the boundary between two media; dispersion is the fact that the amount of bending depends on wavelength. A single colour refracts without dispersing, but white light both refracts and disperses, because its many wavelengths each refract by a slightly different amount.\n\n<\/div><\/details>\n\n<details class=\"pf-faq-item\"><summary>Why do diamonds sparkle with rainbow colours?<\/summary><div class=\"pf-faq-item-answer\">\n\nDiamonds show rainbow flashes, called fire, because diamond has both a very high refractive index (about 2.42) and strong dispersion (0.044). Light entering a cut diamond is bent sharply, totally internally reflected off the back facets, and spread into its colours on the way out, so the returning light flashes red, blue and green.\n\n<\/div><\/details>\n","protected":false},"excerpt":{"rendered":"<p>Dispersion of light is why a glass prism splits white light into a rainbow. Learn why violet bends more than red, the key formulas, and 7 real-world examples.<\/p>\n","protected":false},"author":1,"featured_media":477,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[4],"tags":[295,292,293,294,152],"class_list":["post-476","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-waves","tag-chromatic-aberration","tag-dispersion-of-light","tag-prism","tag-rainbow","tag-refraction"],"_links":{"self":[{"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/posts\/476","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=476"}],"version-history":[{"count":2,"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/posts\/476\/revisions"}],"predecessor-version":[{"id":560,"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/posts\/476\/revisions\/560"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/media\/477"}],"wp:attachment":[{"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/media?parent=476"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/categories?post=476"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/physicsfundamentalsinfo.com\/blog\/wp-json\/wp\/v2\/tags?post=476"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}