رنگین کمان (که با نامهای قوس و قزح، آز فندک، تیراژه، کمان رستم، آدینده یا نوشه نیز شناخته میشود) پدیدهای نوری و قیاسی است که زمانی که خورشید به قطرات نم و رطوبت جو زمین میتابد باعث ایجاد طیفی از نور در آسمان میشود. این پدیده به شکل یک کمان رنگین در میآید.
رنگین کمانها به کمک نور خورشید در آسمان در سوی مخالف خورشید پدیدار میشوند.
در یک رنگینکمان اصلی (رنگینکمان پایینتر، و معمولاً روشنتر) رنگ قرمز در بخش بیرونی (یا بالایی) کمان، و بنفش در بخش درونی دیده میشود. این رنگینکمان دومی ممکن است بالا و بیرون کمان اصلی دیده شود، و ترتیب رنگهایش معکوس شدهاست (رنگ قرمز در هر یک از دو رنگینکمان به سوی دیگری است). این رنگینکمان دوم با دو بار انعکاس نور در قطرات آب بوگوتایی) غیرممکناند، چون انعکاس سوم از نور درون قطرات آب پرتوهایشان را تقریباً در جهت خورشید میتاباند، و از اینرو نامرئی هستند. ممکن است بعضی پدیدهها (نظیر «کمانهای اضافی» خیلی نزدیک و درون کمانهای اصلی) با «رنگینکمانهای سهتایی» اشتباه گرفته شوند. همچنین برای یک ناظر غیرممکن است که برای دیدن رنگینکمان حاصل از قطرات آب در زاویهای غیر از زاویه مرسوم (که ۴۲درجه با جهت مخالف خورشید میسازد) طرحی بریزد. حتی اگر ناظری ناظر دیگری را که بنظر میرسد «زیر» یا «در انتهای» یک رنگینکمان است ببیند، ناظر دوم رنگینکمان متفاوتی را، در همان زاویهای که ناظر اول دیده بود، خواهد دید. از اینرو، یک «رنگینکمان» شیء فیزیکی نیست، و بهطور فیزیکی نمیتوان به آن نزدیک شد.
یک رنگینکمان طیف پیوستهای از رنگها را پوشش میدهد؛ نوارهای متمایز (شامل تعدادی نوار) که ساختهٔ دید رنگی انسان هستند، و هیچ نوع نواربندیی در یک عکس سیاه سفید از رنگینکمان مشاهده نمیشود (فقط گرادیان ملایمی از شدت به یک مقدار بیشینه میرسد، سپس با یک کمینه در طرف دیگر کمان محو میشود). برای رنگهایی که با چشم انسان عادی دیده میشود، توالی ذکر شده و به یاد مانده، در فارسی، هفتتایی قرمز، نارنجی، زرد، سبز، آّبی، نیلی سیر و بنفش است. با این حال افراد کور-رنگ رنگهای کمتری خواهند دید. بجز باران، مه، افشانه، و شبنم معلق در هوا نیز میتوانند رنگینکمان تشکیل دهند.
پدیداری رنگین کمان[ویرایش]
رنگینکمانها را میتوان هر زمان که قطرات آب در هوا وجود دارند و نور خورشید از پشت سر در یک زاویه عمودی کوچک میتابد مشاهده کرد. بخاطر همین رنگین کمانها اغلب در نیمهٔ غربی آسمان به هنگام صبح و در نیمهٔ شرقی آسمان به هنگام عصر دیده میشوند. جلوههای تماشایی رنگین کمانها در زمانی که نیمی از آسمان به خاطر وجود ابرهای در حال بارش تاریک است و ناظر در مکانی با آسمانی صاف و در جهت خورشید قرار دارد، دیده خواهد شد. یک رنگینکمان درخشان با زمینهٔ تاریک. در طی این شرایط خوب دید، اغلب رنگین کمانی بزرگتر ولی کمرنگ تر با فاصلهٔ ۱۰ درجه بیرون از رنگین کمان اصلی و ترتیب رنگی وارونه (نسبت به رنگین کمان اصلی) نمایان میشود
معمولاً در نزدیکی آبشارها و فوارهها نیز اثر رنگینکمان مشاهده میشود. بعلاوه، در طول یک روز آفتابی این اثر را میتوان بهطور مصنوعی با پراکندهساختن قطرههای آب در هوا ایجاد کرد. یک مهتاب کمان، رنگینکمان ماهتابی یا رنگینکمان شبهنگام، را به ندرت در شبهای شدیداً مهتابی میتوان مشاهده کرد. از آنجا که قوهٔ بینایی انسان برای رنگ در نور کم ضعیف است، مهتاب کمانها اغلب سفید مشاهده میشوند. عکاسی از نیمدایرهٔ کامل رنگینکمان در یک فریم مشکل است، چون نیاز به زاویه دید ۸۴درجهاست. برای یک دوربین ۳۵mm، یک عدسی با فاصله کانونی ۱۹mm یا عدسی زاویه-گسترده کمتر مورد نیاز است. حال که نرمافزارهای قدرتمندی برای چسباندن چندین عکس در یک سراسرنما در دسترس است، تصاویر کل کمان و حتی کمانهای ثانویه را میتوان به راحتی از یک سری از فریمهای رویهم افتاده ساخت. از داخل هواپیما، شخص شانس دیدن تمام دایرهٔ رنگینکمان را، با سایهٔ هواپیما در مرکز، دارد. این پدیده میتواند با گلوری اشتباه گرفته شود، اما یک گلوری معمولاً خیلی کوچکتر است، تنها ۲۰–۵درجه را پوشش میدهد.
در شرایط دید خوب (برای مثال، وجود ابر تیره در پشت رنگینکمان)، کمان دوم را با ترتیب رنگ معکوس میتوان دید. در زمینهٔ آسمان آبی، کمان دوم با اشکال قابل رویت است.
رنگینکمان طیف پیوستهای از رنگها را پوشش میدهد- تفکیک ظاهری محصول رنگدانههای نوری در چشم انسان و پردازش عصبی خروجیهای گیرندههای نوریمان در مغز است. از آنجا که قلهٔ پاسخ گیرندههای رنگی انسان از فردی به فرد دیگر تغییر میکند، افراد مختلف اندکی رنگها را متفاوت خواهند دید، و افرادی که کور رنگ هستند تعداد کمتری از رنگها را خواهند دید. با این حال، هفت رنگی که در زیر لیست شدهاند گمان میشود که از این حکایت میکنند که انسانها در هر کجا، با دید رنگی عادی، رنگینکمان را چگونه میبینند. رنگ آخر در رنگینکمان بنفش است، نه ارغوانی.
نیوتن بهطور ابتکاری (۱۶۷۲م) تنها پنج رنگ اصلی را نامگذاری کرد: قرمز، زرد، سبز، آبی و بنفش. نارنجی و نیلی سیر را بعداً اضافه کرد، تا در توافق با تعداد نتها در مقیاسی موسیقایی هفت رنگ را بدهد.
این نوع رنگین کمان بعضی اوقات و به ندرت در موقع طلوع یا غروب خورشید اتفاق میافتد زمانی که نورهایی با طول موج کوتاهتر، مانند رنگ آبی، بنفش و سبز پراکنده شده و از طیفهای مرئی حذف میشوند و تنها نورهای با طول موج بلند (سرخ) دیده میشوند. میتوان علت این پراکندگی را باران دانست که باعث پیدایش پدیده نادر و زیبای تکین کمان میشود.
نور که ابتدا هنگام ورود به سطح قطره باران شکسته شدهاست، در پشت قطره بازتاب میکند، و بار دیگر هنگام ترک قطره میشکند. اثر کلی به گونهای است که نور ورودی در گسترهٔ عریضی از زاویهها، با بیشترین شدت نوری در زاویهٔ ۴۰ تا ۴۲ درجه، بازمیتابد. زاویه مستقل از اندازهٔ قطرهاست، اما به شاخص شکست آن وابستهاست. آب دریا شاخص شکست بزرگتری نسبت به آب باران دارد، از اینرو شعاع «رنگینکمان» در افشانهٔ دریا کوچکتر از یک رنگینکمان واقعی است. این رنگینکمان برای چشم غیر مسلح با چینش از دست رفتهای از این کمانها مشاهده میشود. مقدار شکست نور به طولموجاش، و از اینرو به رنگهایش بستگی دارد. نور آبی (طول موج کوتاهتر) در زاویهٔ بزرگتری نسبت به نور قرمز میشکند، اما بواسطهٔ بازتاب پرتوهای نور از پشت قطره، نور آبی نسبت به نور قرمز هنگام خروج از قطره با زاویهٔ کمتری با پرتو سفید فرودی اصلی میسازد. ممکن است فکر کنید که عجیب است که الگوی رنگها در یک رنگینکمان قرمز را در بیرون کمان و آبی را در درون آن دارد. با اینحال، زمانیکه این موضوع را با دقت بیشتری وارسی کنیم، متوجه میشویم که اگر نور قرمز خارج شده از یک قطره توسط ناظری مشاهده شود، نور آبی آن قطره دیده نخواهد شد زیرا این نور در مسیری متفاوت با نور قرمز حرکت قرار دارد: مسیری که با چشمان ناظر در یک راستا نیست. نور آبی مشاهده شده در این رنگینکمان از قطرهٔ متفاوتی میآید، که بایستی زیر قطرهای باشد که نور قرمز از آن مشاهده میشود.
عکس اعتقاد عموم، نور در پشت قطره باران دستخوش بازتاب کلی نمیشود، و مقداری نور از پشت قطره خارج میشود. با این حال، نور خروجی از پشت قطره باران بین ناظر و خورشید رنگینکمان تشکیل نمیدهد زیرا طیف تابشی از پشت قطره باران بمانند رنگین کمانهای مرئی دارای شدت حداکثری نیستند، و از اینرو رنگها بیشتر از آنکه رنگینکمان تشکیل دهند، با هم ترکیب میشوند.
یک رنگینکمان در واقع در محل مشخصی از آسمان وجود ندارد. محل ظاهر شدنش به محل ناظر و موقعیت خورشید بستگی دارد. تمام قطرات باران نور خورشید را یکسان شکسته و بازمیتابند، اما فقط نور از بعضی قطرات باران به چشم ناظر میرسد. این نور همان است که رنگینکمان را برای ناظر تشکیل میدهد. محل یک رنگینکمان در آسمان نسبت به ناظر همیشه در سوی مخالف خورشید است، و همیشه رنگینکمان درونی روشنتر از رنگینکمان بیرونی است. مرکز کمان سایهٔ سر ناظر است، یا بهطور دقیقتر نقطهٔ پاد خورشیدی (که در طول روز زیر افق است)، در زاویهٔ ۴۰ تا ۴۲درجه نسبت به خط بین سر ناظر و سایهاش ظاهر میشود. در نتیجه، اگر خورشید بالاتر از ۴۲درجه باشد، رنگینکمان زیر خط افق خواهد بود و معمولاً به مقدار کافی قطره باران بین افق (یعنی، ارتفاع چشم) و زمین وجود ندارد، تا رنگینکمان تشکیل دهند. استثناها زمانی رخ میدهند که ارتفاع ناظر از سطح زمین بیشتر شود، برای مثال در یک هواپیما، در بالای کوه، یا بالای یک آبشار.
رنگین کمان تمام دور[ویرایش]
از نظر تئوری همهٔ رنگینکمانها دایرهٔ کامل هستند ولی در روی زمین ما معمولاً فقط نیمهٔ بالایی آنها را میبینیم. از آنجاییکه مرکز رنگینکمان به صورت قطری در طرف مقابل موقعیت خورشید در آسمان است بیشترین مقداری که ما میتوانیم از رنگینکمان ببینیم حدود ۵۰٪ آن است که آنهم در هنگام صبح زود یا غروب که خورشید پایین است قابل مشاهده است. برای اینکه بتوانیم دایرهٔ کامل را ببینیم لازم است که قطرات آب در زیر افق دید بیننده باشند.
وقتی نور خورشید به داخل قطرات باران میتابد آنها به صورت منشورهای کوچکی عمل میکنند که نور را متفرق کرده و به رنگهای مجزا تجزیه میکند. بهترین و شفافترین رنگین کمان زمانی تشکیل میشود که باران خیلی شدید باشد و قطرات بزرگی در آسمان باشند. در واقع پرتوهای نور در هنگام عبور از قطرات آب دو بار خم میشوند. بار اول زمانی است که وارد قطرات آب میشوند و بار دوم هنگامی که از قطرات خارج میشوند.
دلیل دایره بودن رنگینکمان این است که قطرات آب با زاویهٔ بین ۴۰ تا ۴۲ درجه از زاویهٔ ورودشان خارج میشوند و تجمع این پرتوها در هنگام تابیدن نور به قطرات باران باعث میشود که یک دایره تشکیل شود ولی اگر خورشید خیلی پایین باشد مثلاً هنگام صبح یا غروب ما فقط یکنیمه از این کره را میبینیم و هر چه خورشید بالاتر باشد ما مقدار کمتری از دایرهٔ رنگینکمان را میبینیم. تنها راهی که بتوان دایرهٔ کامل رنگینکمان را دید این است که به بالای قطرات باران رفته و خورشید را در پشت سر خود داشته باشیم؛ مثلاً در داخل هواپیما یا بالای یک آبشار میتوان یک رنگینکمان دایرهای کامل را دید.
پیوند به بیرون[ویرایش]
A rainbow is a meteorological phenomenon that is caused by reflection, refraction and dispersion of light in water droplets resulting in a spectrum of light appearing in the sky. It takes the form of a multicoloured circular arc. Rainbows caused by sunlight always appear in the section of sky directly opposite the sun.
Rainbows can be full circles. However, the observer normally sees only an arc formed by illuminated droplets above the ground, and centered on a line from the sun to the observer's eye.
In a primary rainbow, the arc shows red on the outer part and violet on the inner side. This rainbow is caused by light being refracted when entering a droplet of water, then reflected inside on the back of the droplet and refracted again when leaving it.
In a double rainbow, a second arc is seen outside the primary arc, and has the order of its colours reversed, with red on the inner side of the arc. This is caused by the light being reflected twice on the inside of the droplet before leaving it.
A rainbow is not located at a specific distance from the observer, but comes from an optical illusion caused by any water droplets viewed from a certain angle relative to a light source. Thus, a rainbow is not an object and cannot be physically approached. Indeed, it is impossible for an observer to see a rainbow from water droplets at any angle other than the customary one of 42 degrees from the direction opposite the light source. Even if an observer sees another observer who seems "under" or "at the end of" a rainbow, the second observer will see a different rainbow—farther off—at the same angle as seen by the first observer.
Rainbows span a continuous spectrum of colours. Any distinct bands perceived are an artefact of human colour vision, and no banding of any type is seen in a black-and-white photo of a rainbow, only a smooth gradation of intensity to a maximum, then fading towards the other side. For colours seen by the human eye, the most commonly cited and remembered sequence is Newton's sevenfold red, orange, yellow, green, blue, indigo and violet, remembered by the mnemonic Richard Of York Gave Battle In Vain (ROYGBIV).
Rainbows can be caused by many forms of airborne water. These include not only rain, but also mist, spray, and airborne dew.
Rainbows can be observed whenever there are water drops in the air and sunlight shining from behind the observer at a low altitude angle. Because of this, rainbows are usually seen in the western sky during the morning and in the eastern sky during the early evening. The most spectacular rainbow displays happen when half the sky is still dark with raining clouds and the observer is at a spot with clear sky in the direction of the sun. The result is a luminous rainbow that contrasts with the darkened background. During such good visibility conditions, the larger but fainter secondary rainbow is often visible. It appears about 10° outside of the primary rainbow, with inverse order of colours.
The rainbow effect is also commonly seen near waterfalls or fountains. In addition, the effect can be artificially created by dispersing water droplets into the air during a sunny day. Rarely, a moonbow, lunar rainbow or nighttime rainbow, can be seen on strongly moonlit nights. As human visual perception for colour is poor in low light, moonbows are often perceived to be white.
It is difficult to photograph the complete semicircle of a rainbow in one frame, as this would require an angle of view of 84°. For a 35 mm camera, a wide-angle lens with a focal length of 19 mm or less would be required. Now that software for stitching several images into a panorama is available, images of the entire arc and even secondary arcs can be created fairly easily from a series of overlapping frames.
From above the earth such as in an aeroplane, it is sometimes possible to see a rainbow as a full circle. This phenomenon can be confused with the glory phenomenon, but a glory is usually much smaller, covering only 5–20°.
The sky inside a primary rainbow is brighter than the sky outside of the bow. This is because each raindrop is a sphere and it scatters light over an entire circular disc in the sky. The radius of the disc depends on the wavelength of light, with red light being scattered over a larger angle than blue light. Over most of the disc, scattered light at all wavelengths overlaps, resulting in white light which brightens the sky. At the edge, the wavelength dependence of the scattering gives rise to the rainbow.
Number of colours in spectrum or rainbow
A spectrum obtained using a glass prism and a point source is a continuum of wavelengths without bands. The number of colours that the human eye is able to distinguish in a spectrum is in the order of 100. Accordingly, the Munsell colour system (a 20th-century system for numerically describing colours, based on equal steps for human visual perception) distinguishes 100 hues. The apparent discreteness of main colours is an artefact of human perception and the exact number of main colours is a somewhat arbitrary choice.
Newton, who admitted his eyes were not very critical in distinguishing colours, originally (1672) divided the spectrum into five main colours: red, yellow, green, blue and violet. Later he included orange and indigo, giving seven main colours by analogy to the number of notes in a musical scale. Newton chose to divide the visible spectrum into seven colours out of a belief derived from the beliefs of the ancient Greek sophists, who thought there was a connection between the colours, the musical notes, the known objects in the Solar System, and the days of the week. Scholars have noted that what Newton regarded at the time as "blue" would today be regarded as cyan, and what Newton called "indigo" would today be considered blue.
According to Isaac Asimov, "It is customary to list indigo as a colour lying between blue and violet, but it has never seemed to me that indigo is worth the dignity of being considered a separate colour. To my eyes it seems merely deep blue."
The colour pattern of a rainbow is different from a spectrum, and the colours are less saturated. There is spectral smearing in a rainbow owing to the fact that for any particular wavelength, there is a distribution of exit angles, rather than a single unvarying angle. In addition, a rainbow is a blurred version of the bow obtained from a point source, because the disk diameter of the sun (0.5°) cannot be neglected compared to the width of a rainbow (2°). Further red of the first supplementary rainbow overlaps the violet of the primary rainbow, so rather than the final colour being a variant of spectral violet, it is actually a purple. The number of colour bands of a rainbow may therefore be different from the number of bands in a spectrum, especially if the droplets are particularly large or small. Therefore, the number of colours of a rainbow is variable. If, however, the word rainbow is used inaccurately to mean spectrum, it is the number of main colours in the spectrum.
The question of whether everyone sees seven colours in a rainbow is related to the idea of linguistic relativity. Suggestions have been made that there is universality in the way that a rainbow is perceived. However, more recent research suggests that the number of distinct colours observed and what these are called depend on the language that one uses, with people whose language has fewer colour words seeing fewer discrete colour bands.
When sunlight encounters a raindrop, part of the light is reflected and the rest enters the raindrop. The light is refracted at the surface of the raindrop. When this light hits the back of the raindrop, some of it is reflected off the back. When the internally reflected light reaches the surface again, once more some is internally reflected and some is refracted as it exits the drop. (The light that reflects off the drop, exits from the back, or continues to bounce around inside the drop after the second encounter with the surface, is not relevant to the formation of the primary rainbow.) The overall effect is that part of the incoming light is reflected back over the range of 0° to 42°, with the most intense light at 42°. This angle is independent of the size of the drop, but does depend on its refractive index. Seawater has a higher refractive index than rain water, so the radius of a "rainbow" in sea spray is smaller than a true rainbow. This is visible to the naked eye by a misalignment of these bows.
The reason the returning light is most intense at about 42° is that this is a turning point – light hitting the outermost ring of the drop gets returned at less than 42°, as does the light hitting the drop nearer to its centre. There is a circular band of light that all gets returned right around 42°. If the sun were a laser emitting parallel, monochromatic rays, then the luminance (brightness) of the bow would tend toward infinity at this angle (ignoring interference effects). (See Caustic (optics).) But since the sun's luminance is finite and its rays are not all parallel (it covers about half a degree of the sky) the luminance does not go to infinity. Furthermore, the amount by which light is refracted depends upon its wavelength, and hence its colour. This effect is called dispersion. Blue light (shorter wavelength) is refracted at a greater angle than red light, but due to the reflection of light rays from the back of the droplet, the blue light emerges from the droplet at a smaller angle to the original incident white light ray than the red light. Due to this angle, blue is seen on the inside of the arc of the primary rainbow, and red on the outside. The result of this is not only to give different colours to different parts of the rainbow, but also to diminish the brightness. (A "rainbow" formed by droplets of a liquid with no dispersion would be white, but brighter than a normal rainbow.)
The light at the back of the raindrop does not undergo total internal reflection, and some light does emerge from the back. However, light coming out the back of the raindrop does not create a rainbow between the observer and the sun because spectra emitted from the back of the raindrop do not have a maximum of intensity, as the other visible rainbows do, and thus the colours blend together rather than forming a rainbow.
A rainbow does not exist at one particular location. Many rainbows exist; however, only one can be seen depending on the particular observer's viewpoint as droplets of light illuminated by the sun. All raindrops refract and reflect the sunlight in the same way, but only the light from some raindrops reaches the observer's eye. This light is what constitutes the rainbow for that observer. The whole system composed by the sun's rays, the observer's head, and the (spherical) water drops has an axial symmetry around the axis through the observer's head and parallel to the sun's rays. The rainbow is curved because the set of all the raindrops that have the right angle between the observer, the drop, and the sun, lie on a cone pointing at the sun with the observer at the tip. The base of the cone forms a circle at an angle of 40–42° to the line between the observer's head and their shadow but 50% or more of the circle is below the horizon, unless the observer is sufficiently far above the earth's surface to see it all, for example in an aeroplane (see above). Alternatively, an observer with the right vantage point may see the full circle in a fountain or waterfall spray.
It is possible to determine the perceived angle which the rainbow subtends as follows.
Given a spherical raindrop, and defining the perceived angle of the rainbow as 2φ, and the angle of the internal reflection as 2β, then the angle of incidence of the sun's rays with respect to the drop's surface normal is 2β − φ. Since the angle of refraction is β, Snell's law gives us
where n = 1.333 is the refractive index of water. Solving for φ, we get
The rainbow will occur where the angle φ is maximum with respect to the angle β. Therefore, from calculus, we can set dφ/dβ = 0, and solve for β, which yields
Substituting back into the earlier equation for φ yields 2φmax ≈ 42° as the radius angle of the rainbow.
The term double rainbow is used when both the primary and secondary rainbows are visible. In theory, all rainbows are double rainbows, but since the secondary bow is always fainter than the primary, it may be too weak to spot in practice.
Secondary rainbows are caused by a double reflection of sunlight inside the water droplets. Technically the secondary bow is centred on the sun itself, but since its angular size is more than 90° (about 127° for violet to 130° for red), it is seen on the same side of the sky as the primary rainbow, about 10° outside it at an apparent angle of 50–53°. As a result of the "inside" of the secondary bow being "up" to the observer, the colours appear reversed compared to those of the primary bow.
The secondary rainbow is fainter than the primary because more light escapes from two reflections compared to one and because the rainbow itself is spread over a greater area of the sky. Each rainbow reflects white light inside its coloured bands, but that is "down" for the primary and "up" for the secondary. The dark area of unlit sky lying between the primary and secondary bows is called Alexander's band, after Alexander of Aphrodisias who first described it.
Unlike a double rainbow that consists of two separate and concentric rainbow arcs, the very rare twinned rainbow appears as two rainbow arcs that split from a single base. The colours in the second bow, rather than reversing as in a secondary rainbow, appear in the same order as the primary rainbow. A "normal" secondary rainbow may be present as well. Twinned rainbows can look similar to, but should not be confused with supernumerary bands. The two phenomena may be told apart by their difference in colour profile: supernumerary bands consist of subdued pastel hues (mainly pink, purple and green), while the twinned rainbow shows the same spectrum as a regular rainbow. The cause of a twinned rainbow is the combination of different sizes of water drops falling from the sky. Due to air resistance, raindrops flatten as they fall, and flattening is more prominent in larger water drops. When two rain showers with different-sized raindrops combine, they each produce slightly different rainbows which may combine and form a twinned rainbow. A numerical ray tracing study showed that a twinned rainbow on a photo could be explained by a mixture of 0.40 and 0.45 mm droplets. That small difference in droplet size resulted in a small difference in flattening of the droplet shape, and a large difference in flattening of the rainbow top.
Meanwhile, the even rarer case of a rainbow split into three branches was observed and photographed in nature.
In theory, every rainbow is a circle, but from the ground, usually only its upper half can be seen. Since the rainbow's centre is diametrically opposed to the sun's position in the sky, more of the circle comes into view as the sun approaches the horizon, meaning that the largest section of the circle normally seen is about 50% during sunset or sunrise. Viewing the rainbow's lower half requires the presence of water droplets below the observer's horizon, as well as sunlight that is able to reach them. These requirements are not usually met when the viewer is at ground level, either because droplets are absent in the required position, or because the sunlight is obstructed by the landscape behind the observer. From a high viewpoint such as a high building or an aircraft, however, the requirements can be met and the full-circle rainbow can be seen. Like a partial rainbow, the circular rainbow can have a secondary bow or supernumerary bows as well. It is possible to produce the full circle when standing on the ground, for example by spraying a water mist from a garden hose while facing away from the sun.
A circular rainbow should not be confused with the glory, which is much smaller in diameter and is created by different optical processes. In the right circumstances, a glory and a (circular) rainbow or fog bow can occur together. Another atmospheric phenomenon that may be mistaken for a "circular rainbow" is the 22° halo, which is caused by ice crystals rather than liquid water droplets, and is located around the sun (or moon), not opposite it.
In certain circumstances, one or several narrow, faintly coloured bands can be seen bordering the violet edge of a rainbow; i.e., inside the primary bow or, much more rarely, outside the secondary. These extra bands are called supernumerary rainbows or supernumerary bands; together with the rainbow itself the phenomenon is also known as a stacker rainbow. The supernumerary bows are slightly detached from the main bow, become successively fainter along with their distance from it, and have pastel colours (consisting mainly of pink, purple and green hues) rather than the usual spectrum pattern. The effect becomes apparent when water droplets are involved that have a diameter of about 1 mm or less; the smaller the droplets are, the broader the supernumerary bands become, and the less saturated their colours. Due to their origin in small droplets, supernumerary bands tend to be particularly prominent in fogbows.
Supernumerary rainbows cannot be explained using classical geometric optics. The alternating faint bands are caused by interference between rays of light following slightly different paths with slightly varying lengths within the raindrops. Some rays are in phase, reinforcing each other through constructive interference, creating a bright band; others are out of phase by up to half a wavelength, cancelling each other out through destructive interference, and creating a gap. Given the different angles of refraction for rays of different colours, the patterns of interference are slightly different for rays of different colours, so each bright band is differentiated in colour, creating a miniature rainbow. Supernumerary rainbows are clearest when raindrops are small and of uniform size. The very existence of supernumerary rainbows was historically a first indication of the wave nature of light, and the first explanation was provided by Thomas Young in 1804.
Reflected rainbow, reflection rainbow
When a rainbow appears above a body of water, two complementary mirror bows may be seen below and above the horizon, originating from different light paths. Their names are slightly different.
A reflected rainbow may appear in the water surface below the horizon. The sunlight is first deflected by the raindrops, and then reflected off the body of water, before reaching the observer. The reflected rainbow is frequently visible, at least partially, even in small puddles.
A reflection rainbow may be produced where sunlight reflects off a body of water before reaching the raindrops), if the water body is large, quiet over its entire surface, and close to the rain curtain. The reflection rainbow appears above the horizon. It intersects the normal rainbow at the horizon, and its arc reaches higher in the sky, with its centre as high above the horizon as the normal rainbow's centre is below it. Due to the combination of requirements, a reflection rainbow is rarely visible.
Up to eight separate bows may be distinguished if the reflected and reflection rainbows happen to occur simultaneously: The normal (non-reflection) primary and secondary bows above the horizon (1, 2) with their reflected counterparts below it (3, 4), and the reflection primary and secondary bows above the horizon (5, 6) with their reflected counterparts below it (7, 8).
Occasionally a shower may happen at sunrise or sunset, where the shorter wavelengths like blue and green have been scattered and essentially removed from the spectrum. Further scattering may occur due to the rain, and the result can be the rare and dramatic monochrome or red rainbow.
In addition to the common primary and secondary rainbows, it is also possible for rainbows of higher orders to form. The order of a rainbow is determined by the number of light reflections inside the water droplets that create it: One reflection results in the first-order or primary rainbow; two reflections create the second-order or secondary rainbow. More internal reflections cause bows of higher orders—theoretically unto infinity. As more and more light is lost with each internal reflection, however, each subsequent bow becomes progressively dimmer and therefore increasingly harder to spot. An additional challenge in observing the third-order (or tertiary) and fourth-order (quaternary) rainbows is their location in the direction of the sun (about 40° and 45° from the sun, respectively), causing them to become drowned in its glare.
For these reasons, naturally occurring rainbows of an order higher than 2 are rarely visible to the naked eye. Nevertheless, sightings of the third-order bow in nature have been reported, and in 2011 it was photographed definitively for the first time. Shortly after, the fourth-order rainbow was photographed as well, and in 2014 the first ever pictures of the fifth-order (or quinary) rainbow, located in between the primary and secondary bows, were published.
In a laboratory setting, it is possible to create bows of much higher orders. Felix Billet (1808–1882) depicted angular positions up to the 19th-order rainbow, a pattern he called a "rose of rainbows". In the laboratory, it is possible to observe higher-order rainbows by using extremely bright and well collimated light produced by lasers. Up to the 200th-order rainbow was reported by Ng et al. in 1998 using a similar method but an argon ion laser beam.
Tertiary and quaternary rainbows should not be confused with "triple" and "quadruple" rainbows—terms sometimes erroneously used to refer to the—much more common—supernumerary bows and reflection rainbows.
Rainbows under moonlight
Like most atmospheric optical phenomena, rainbows can be caused by light from the Sun, but also from the Moon. In case of the latter, the rainbow is referred to as a lunar rainbow or moonbow. They are much dimmer and rarer than solar rainbows, requiring the Moon to be near-full in order for them to be seen. For the same reason, moonbows are often perceived as white and may be thought of as monochrome. The full spectrum is present, however, but the human eye is not normally sensitive enough to see the colours. Long exposure photographs will sometimes show the colour in this type of rainbow.
Fogbows form in the same way as rainbows, but they are formed by much smaller cloud and fog droplets that diffract light extensively. They are almost white with faint reds on the outside and blues inside; often one or more broad supernumerary bands can be discerned inside the inner edge. The colours are dim because the bow in each colour is very broad and the colours overlap. Fogbows are commonly seen over water when air in contact with the cooler water is chilled, but they can be found anywhere if the fog is thin enough for the sun to shine through and the sun is fairly bright. They are very large—almost as big as a rainbow and much broader. They sometimes appear with a glory at the bow's centre.
Circumhorizontal and circumzenithal arcs
The circumzenithal and circumhorizontal arcs are two related optical phenomena similar in appearance to a rainbow, but unlike the latter, their origin lies in light refraction through hexagonal ice crystals rather than liquid water droplets. This means that they are not rainbows, but members of the large family of halos.
Both arcs are brightly coloured ring segments centred on the zenith, but in different positions in the sky: The circumzenithal arc is notably curved and located high above the Sun (or Moon) with its convex side pointing downwards (creating the impression of an "upside down rainbow"); the circumhorizontal arc runs much closer to the horizon, is more straight and located at a significant distance below the Sun (or Moon). Both arcs have their red side pointing towards the sun and their violet part away from it, meaning the circumzenithal arc is red on the bottom, while the circumhorizontal arc is red on top.
The circumhorizontal arc is sometimes referred to by the misnomer "fire rainbow". In order to view it, the Sun or Moon must be at least 58° above the horizon, making it a rare occurrence at higher latitudes. The circumzenithal arc, visible only at a solar or lunar elevation of less than 32°, is much more common, but often missed since it occurs almost directly overhead.
Rainbows on Titan
It has been suggested that rainbows might exist on Saturn's moon Titan, as it has a wet surface and humid clouds. The radius of a Titan rainbow would be about 49° instead of 42°, because the fluid in that cold environment is methane instead of water. Although visible rainbows may be rare due to Titan's hazy skies, infrared rainbows may be more common, but an observer would need infrared night vision goggles to see them.
Rainbows with different materials
Droplets (or spheres) composed of materials with different refractive indices than plain water produce rainbows with different radius angles. Since salt water has a higher refractive index, a sea spray bow doesn't perfectly align with the ordinary rainbow, if seen at the same spot. Tiny plastic or glass marbles may be used in road marking as a reflectors to enhance its visibility by drivers at night. Due to a much higher refractive index, rainbows observed on such marbles have a noticeably smaller radius. One can easily reproduce such phenomena by sprinkling liquids of different refractive indices in the air, as illustrated in the photo.
The displacement of the rainbow due to different refractive indices can be pushed to a peculiar limit. For a material with a refractive index larger than 2, there is no angle fulfilling the requirements for the first order rainbow. For example, the index of refraction of diamond is about 2.4, so diamond spheres would produce rainbows starting from the second order, omitting the first order. In general, as the refractive index exceeds a number n+1, where n is a natural number, the critical incidence angle for n times internally reflected rays escapes the domain . This results in a rainbow of the n-th order shrinking to the antisolar point and vanishing.
The classical Greek scholar Aristotle (384–322 BC) was first to devote serious attention to the rainbow. According to Raymond L. Lee and Alistair B. Fraser, "Despite its many flaws and its appeal to Pythagorean numerology, Aristotle's qualitative explanation showed an inventiveness and relative consistency that was unmatched for centuries. After Aristotle's death, much rainbow theory consisted of reaction to his work, although not all of this was uncritical."
In Book I of Naturales Quaestiones (c. 65 AD), the Roman philosopher Seneca the Younger discusses various theories of the formation of rainbows extensively, including those of Aristotle. He notices that rainbows appear always opposite to the sun, that they appear in water sprayed by a rower, in the water spat by a fuller on clothes stretched on pegs or by water sprayed through a small hole in a burst pipe. He even speaks of rainbows produced by small rods (virgulae) of glass, anticipating Newton's experiences with prisms. He takes into account two theories: one, that the rainbow is produced by the sun reflecting in each water drop, the other, that it is produced by the sun reflected in a cloud shaped like a concave mirror; he favours the latter. He also discusses other phenomena related to rainbows: the mysterious "virgae" (rods), halos and parhelia.
According to Hüseyin Gazi Topdemir, the Arab physicist and polymath Ibn al-Haytham (Alhazen; 965–1039), attempted to provide a scientific explanation for the rainbow phenomenon. In his Maqala fi al-Hala wa Qaws Quzah (On the Rainbow and Halo), al-Haytham "explained the formation of rainbow as an image, which forms at a concave mirror. If the rays of light coming from a farther light source reflect to any point on axis of the concave mirror, they form concentric circles in that point. When it is supposed that the sun as a farther light source, the eye of viewer as a point on the axis of mirror and a cloud as a reflecting surface, then it can be observed the concentric circles are forming on the axis." He was not able to verify this because his theory that "light from the sun is reflected by a cloud before reaching the eye" did not allow for a possible experimental verification. This explanation was repeated by Averroes, and, though incorrect, provided the groundwork for the correct explanations later given by Kamāl al-Dīn al-Fārisī in 1309 and, independently, by Theodoric of Freiberg (c. 1250–c. 1311)—both having studied al-Haytham's Book of Optics.
Ibn al-Haytham's contemporary, the Persian philosopher and polymath Ibn Sīnā (Avicenna; 980–1037), provided an alternative explanation, writing "that the bow is not formed in the dark cloud but rather in the very thin mist lying between the cloud and the sun or observer. The cloud, he thought, serves simply as the background of this thin substance, much as a quicksilver lining is placed upon the rear surface of the glass in a mirror. Ibn Sīnā would change the place not only of the bow, but also of the colour formation, holding the iridescence to be merely a subjective sensation in the eye." This explanation, however, was also incorrect. Ibn Sīnā's account accepts many of Aristotle's arguments on the rainbow.
In Song Dynasty China (960–1279), a polymath scholar-official named Shen Kuo (1031–1095) hypothesised—as a certain Sun Sikong (1015–1076) did before him—that rainbows were formed by a phenomenon of sunlight encountering droplets of rain in the air. Paul Dong writes that Shen's explanation of the rainbow as a phenomenon of atmospheric refraction "is basically in accord with modern scientific principles."
According to Nader El-Bizri, the Persian astronomer, Qutb al-Din al-Shirazi (1236–1311), gave a fairly accurate explanation for the rainbow phenomenon. This was elaborated on by his student, Kamāl al-Dīn al-Fārisī (1267–1319), who gave a more mathematically satisfactory explanation of the rainbow. He "proposed a model where the ray of light from the sun was refracted twice by a water droplet, one or more reflections occurring between the two refractions." An experiment with a water-filled glass sphere was conducted and al-Farisi showed the additional refractions due to the glass could be ignored in his model. As he noted in his Kitab Tanqih al-Manazir (The Revision of the Optics), al-Farisi used a large clear vessel of glass in the shape of a sphere, which was filled with water, in order to have an experimental large-scale model of a rain drop. He then placed this model within a camera obscura that has a controlled aperture for the introduction of light. He projected light unto the sphere and ultimately deduced through several trials and detailed observations of reflections and refractions of light that the colours of the rainbow are phenomena of the decomposition of light.
In Europe, Ibn al-Haytham's Book of Optics was translated into Latin and studied by Robert Grosseteste. His work on light was continued by Roger Bacon, who wrote in his Opus Majus of 1268 about experiments with light shining through crystals and water droplets showing the colours of the rainbow. In addition, Bacon was the first to calculate the angular size of the rainbow. He stated that the rainbow summit can not appear higher than 42° above the horizon. Theodoric of Freiberg is known to have given an accurate theoretical explanation of both the primary and secondary rainbows in 1307. He explained the primary rainbow, noting that "when sunlight falls on individual drops of moisture, the rays undergo two refractions (upon ingress and egress) and one reflection (at the back of the drop) before transmission into the eye of the observer." He explained the secondary rainbow through a similar analysis involving two refractions and two reflections.
Descartes' 1637 treatise, Discourse on Method, further advanced this explanation. Knowing that the size of raindrops did not appear to affect the observed rainbow, he experimented with passing rays of light through a large glass sphere filled with water. By measuring the angles that the rays emerged, he concluded that the primary bow was caused by a single internal reflection inside the raindrop and that a secondary bow could be caused by two internal reflections. He supported this conclusion with a derivation of the law of refraction (subsequently to, but independently of, Snell) and correctly calculated the angles for both bows. His explanation of the colours, however, was based on a mechanical version of the traditional theory that colours were produced by a modification of white light.
Isaac Newton demonstrated that white light was composed of the light of all the colours of the rainbow, which a glass prism could separate into the full spectrum of colours, rejecting the theory that the colours were produced by a modification of white light. He also showed that red light is refracted less than blue light, which led to the first scientific explanation of the major features of the rainbow. Newton's corpuscular theory of light was unable to explain supernumerary rainbows, and a satisfactory explanation was not found until Thomas Young realised that light behaves as a wave under certain conditions, and can interfere with itself.
Young's work was refined in the 1820s by George Biddell Airy, who explained the dependence of the strength of the colours of the rainbow on the size of the water droplets. Modern physical descriptions of the rainbow are based on Mie scattering, work published by Gustav Mie in 1908. Advances in computational methods and optical theory continue to lead to a fuller understanding of rainbows. For example, Nussenzveig provides a modern overview.
Experiments on the rainbow phenomenon using artificial raindrops, i.e. water-filled spherical flasks, go back at least to Theodoric of Freiberg in the 14th century. Later, also Descartes studied the phenomenon using a Florence flask. A flask experiment known as Florence's rainbow is still often used today as an imposing and intuitively accessible demonstration experiment of the rainbow phenomenon. It consists in illuminating (with parallel white light) a water-filled spherical flask through a hole in a screen. A rainbow will then appear thrown back / projected on the screen, provided the screen is large enough. Due to the finite wall thickness and the macroscopic character of the artificial raindrop, several subtle differences exist as compared to the natural phenomenon, including slightly changed rainbow angles and a splitting of the rainbow orders.
A very similar experiment consists in using a cylindrical glass vessel filled with water or a solid transparent cylinder and illuminated either parallel to the circular base (i.e. light rays remaining at a fixed height while they transit the cylinder) or under an angle to the base. Under these latter conditions the rainbow angles change relative to the natural phenomenon since the effective index of refraction of water changes (Bravais' index of refraction for inclined rays applies).
Rainbows occur frequently in mythology, and have been used in the arts. One of the earliest literary occurrences of a rainbow is in the Book of Genesis chapter 9, as part of the flood story of Noah, where it is a sign of God's covenant to never destroy all life on earth with a global flood again. In Norse mythology, the rainbow bridge Bifröst connects the world of men (Midgard) and the realm of the gods (Asgard). Cuchavira was the god of the rainbow for the Muisca in present-day Colombia and when the regular rains on the Bogotá savanna were over, the people thanked him offering gold, snails and small emeralds. The Irish leprechaun's secret hiding place for his pot of gold is usually said to be at the end of the rainbow. This place is appropriately impossible to reach, because the rainbow is an optical effect which cannot be approached.
Rainbows appear in heraldry - in heraldry the rainbow proper consists of 4 bands of color (Or, Gules, Vert, Argent) with the ends resting on clouds. Generalised examples in coat of arms include those of the towns of Regen or Pfreimd, both in Bavaria, Germany; and of Bouffémont, France; and of the 69th Infantry Regiment (New York) of the Army National Guard (USA).
Rainbow flags have been used for centuries. It was a symbol of the Cooperative movement in the German Peasants' War in the 16th century, of peace in Italy, and of gay pride and LGBT social movements since the 1970s. In 1994, Archbishop Desmond Tutu and President Nelson Mandela described newly democratic post-apartheid South Africa as the rainbow nation. The rainbow has also been used in technology product logos, including the Apple computer logo. Many political alliances spanning multiple political parties have called themselves a "Rainbow Coalition".