{"id":3696,"date":"2015-06-16T14:02:26","date_gmt":"2015-06-16T14:02:26","guid":{"rendered":"http:\/\/www.swatlibraries.org\/projects\/speed\/anna\/2015\/06\/16\/radiometer\/"},"modified":"2024-01-19T19:10:49","modified_gmt":"2024-01-19T19:10:49","slug":"radiometer","status":"publish","type":"post","link":"https:\/\/demos.swarthmore.edu\/physics\/2015\/06\/radiometer\/","title":{"rendered":"Radiometer"},"content":{"rendered":"<p>&nbsp;<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter\" src=\"\/physics\/wp-content\/uploads\/sites\/2\/2015\/06\/radiometer.jpg\" alt=\"Radiometer Demo Picture\" width=\"337\" height=\"253\" \/><\/p>\n<ul>\n<li><span style=\"font-size: large;\">Temperature difference at edge of metal vanes causes rotor<br \/>\nto spin.<\/span><\/li>\n<li><span style=\"font-size: large;\">Located in L02, section C3<\/span><\/li>\n<li><span style=\"font-size: large;\">Below explanation taken from Wikipedia (so it must be true).<\/span><\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n<p>&#8211;Explanations for\u00a0<span style=\"font-family: 'Baskerville Semibold'; font-size: large; line-height: 1.5;\">the force on the vanes&#8211;<\/span><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"font-family: 'Baskerville Semibold';\">Over the years, there have been many attempts<br \/>\nto explain how a Crookes radiometer works:<\/span><\/p>\n<p>&nbsp;<\/p>\n<p>1. Crookes incorrectly suggested that the force was due to the pressure of light.<br \/>\nThis theory was originally supported by James Clerk Maxwell who had predicted<br \/>\nthis force. This explanation is still often seen in leaflets packaged with the<br \/>\ndevice. The first experiment to disprove this theory was done by Arthur Schuster<br \/>\nin 1876, who observed that there was a force on the glass bulb of the Crookes<br \/>\nradiometer that was in the opposite direction to the rotation of the vanes.<br \/>\nThis showed that the force turning the vanes was generated inside the radiometer.<br \/>\nIf light pressure was the cause of the rotation, then the better the vacuum<br \/>\nin the bulb, the less air resistance to movement, and the faster the vanes should<br \/>\nspin. In 1901, with a better vacuum pump, Pyotr Lebedev showed that in fact,<br \/>\nthe radiometer only works when there is low pressure gas in the bulb, and the<br \/>\nvanes stay motionless in a hard vacuum. Finally, if light pressure were the<br \/>\nmotive force, the radiometer would spin in the opposite direction as the photons<br \/>\non the shiny side being reflected would deposit more momentum than on the black<br \/>\nside where the photons are absorbed. The actual pressure exerted by light is<br \/>\nfar too small to move these vanes but can be measured with devices such as the<br \/>\nNichols radiometer.<\/p>\n<p>&nbsp;<\/p>\n<p>2. Another incorrect theory was that the heat on the dark side was causing the<br \/>\nmaterial to outgas, which pushed the radiometer around. This was effectively<br \/>\ndisproved by both Schuster&#8217;s and Lebedev&#8217;s experiments.<\/p>\n<p>&nbsp;<\/p>\n<p>3. A partial explanation is that gas molecules hitting the warmer side of the<br \/>\nvane will pick up some of the heat, bouncing off the vane with increased speed.<br \/>\nGiving the molecule this extra boost effectively means that a minute pressure<br \/>\nis exerted on the vane. The imbalance of this effect between the warmer black<br \/>\nside and the cooler silver side means the net pressure on the vane is equivalent<br \/>\nto a push on the black side, and as a result the vanes spin round with the black<br \/>\nside trailing. The problem with this idea is that while the faster moving molecules<br \/>\nproduce more force, they also do a better job of stopping other molecules from<br \/>\nreaching the vane, so the net force on the vane should be exactly the same \u2014<br \/>\nthe greater temperature causes a decrease in local density which results in<br \/>\nthe same force on both sides. Years after this explanation was dismissed, Albert<br \/>\nEinstein showed that the two pressures do not cancel out exactly at the edges<br \/>\nof the vanes because of the temperature difference there. The force predicted<br \/>\nby Einstein would be enough to move the vanes, but not fast enough.<\/p>\n<p>&nbsp;<\/p>\n<p>4. The final piece of the puzzle, thermal transpiration, was theorized by Osborne<br \/>\nReynolds, but first published by James Clerk Maxwell in the last paper before<br \/>\nhis death in 1879. Reynolds found that if a porous plate is kept hotter on one<br \/>\nside than the other, the interactions between gas molecules and the plates are<br \/>\nsuch that gas will flow through from the cooler to the hotter side. The vanes<br \/>\nof a typical Crookes radiometer are not porous, but the space past their edges<br \/>\nbehave like the pores in Reynolds&#8217;s plate. On average, the gas molecules move<br \/>\nfrom the cold side toward the hot side whenever the pressure ratio is less than<br \/>\nthe square root of the (absolute) temperature ratio. The pressure difference<br \/>\ncauses the vane to move cold (white) side forward.<\/p>\n<p>Both Einstein&#8217;s and Reynolds&#8217;s forces appear to cause a Crookes radiometer to<br \/>\nrotate, although it still isn&#8217;t clear which one is stronger.<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>&nbsp; Temperature difference at edge of metal vanes causes rotor to spin. Located in L02, section C3 Below explanation taken from Wikipedia (so it must be true). &nbsp; &#8211;Explanations for\u00a0the force on the vanes&#8211; &nbsp; Over the years, there have been many attempts to explain how a Crookes radiometer works: &nbsp; 1. Crookes incorrectly suggested &hellip; <a href=\"https:\/\/demos.swarthmore.edu\/physics\/2015\/06\/radiometer\/\" class=\"more-link\">Continue reading <span class=\"screen-reader-text\">Radiometer<\/span><\/a><\/p>\n","protected":false},"author":4,"featured_media":4794,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[12],"tags":[412],"_links":{"self":[{"href":"https:\/\/demos.swarthmore.edu\/physics\/wp-json\/wp\/v2\/posts\/3696"}],"collection":[{"href":"https:\/\/demos.swarthmore.edu\/physics\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/demos.swarthmore.edu\/physics\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/demos.swarthmore.edu\/physics\/wp-json\/wp\/v2\/users\/4"}],"replies":[{"embeddable":true,"href":"https:\/\/demos.swarthmore.edu\/physics\/wp-json\/wp\/v2\/comments?post=3696"}],"version-history":[{"count":1,"href":"https:\/\/demos.swarthmore.edu\/physics\/wp-json\/wp\/v2\/posts\/3696\/revisions"}],"predecessor-version":[{"id":5455,"href":"https:\/\/demos.swarthmore.edu\/physics\/wp-json\/wp\/v2\/posts\/3696\/revisions\/5455"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/demos.swarthmore.edu\/physics\/wp-json\/wp\/v2\/media\/4794"}],"wp:attachment":[{"href":"https:\/\/demos.swarthmore.edu\/physics\/wp-json\/wp\/v2\/media?parent=3696"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/demos.swarthmore.edu\/physics\/wp-json\/wp\/v2\/categories?post=3696"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/demos.swarthmore.edu\/physics\/wp-json\/wp\/v2\/tags?post=3696"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}