{"id":1781,"date":"2016-08-23T20:43:44","date_gmt":"2016-08-24T00:43:44","guid":{"rendered":"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/?page_id=1781"},"modified":"2017-04-27T11:24:32","modified_gmt":"2017-04-27T15:24:32","slug":"lab-3-background","status":"publish","type":"page","link":"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/lab-3-polarization-of-light\/lab-3-background\/","title":{"rendered":"Background"},"content":{"rendered":"<p>Suppose that we want to specify the orientation of a plane electromagnetic wave in space (this could be helpful for understanding radio reception, to pick a random example).\u00a0 Plane electromagnetic waves are transverse waves, so we know that the electric and magnetic field vectors are oscillating perpendicularly to the direction of travel, as shown in <a href=\"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/lab-3-polarization-of-light\/lab-3-background\/#Fig1\">Fig. 1<\/a>.<\/p>\n<div id=\"attachment_1835\" style=\"width: 739px\" class=\"wp-caption alignnone\"><img loading=\"lazy\" decoding=\"async\" aria-describedby=\"caption-attachment-1835\" id=\"Fig1\" class=\"wp-image-1835 size-full\" src=\"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-content\/uploads\/sites\/105\/2016\/08\/EMWave2.png\" alt=\"EMWave2\" width=\"729\" height=\"388\" srcset=\"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-content\/uploads\/sites\/105\/2016\/08\/EMWave2.png 729w, https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-content\/uploads\/sites\/105\/2016\/08\/EMWave2-150x80.png 150w, https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-content\/uploads\/sites\/105\/2016\/08\/EMWave2-300x160.png 300w, https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-content\/uploads\/sites\/105\/2016\/08\/EMWave2-624x332.png 624w\" sizes=\"auto, (max-width: 729px) 100vw, 729px\" \/><p id=\"caption-attachment-1835\" class=\"wp-caption-text\">Figure 1: An electromagnetic wave<\/p><\/div>\n<p>We also know that the electric and magnetic field vectors are perpendicular to each other, but that still leaves an infinite number of options for orienting the wave.\u00a0 Here are just two more possibilities:<\/p>\n<div id=\"attachment_1832\" style=\"width: 768px\" class=\"wp-caption alignnone\"><img loading=\"lazy\" decoding=\"async\" aria-describedby=\"caption-attachment-1832\" id=\"Fig2\" class=\"wp-image-1832 size-full\" src=\"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-content\/uploads\/sites\/105\/2016\/08\/EMWave1.png\" alt=\"EMWave1\" width=\"758\" height=\"408\" srcset=\"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-content\/uploads\/sites\/105\/2016\/08\/EMWave1.png 758w, https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-content\/uploads\/sites\/105\/2016\/08\/EMWave1-150x81.png 150w, https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-content\/uploads\/sites\/105\/2016\/08\/EMWave1-300x161.png 300w, https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-content\/uploads\/sites\/105\/2016\/08\/EMWave1-624x336.png 624w\" sizes=\"auto, (max-width: 758px) 100vw, 758px\" \/><p id=\"caption-attachment-1832\" class=\"wp-caption-text\">Figure 2: Another electromagnetic wave<\/p><\/div>\n<div id=\"attachment_1837\" style=\"width: 748px\" class=\"wp-caption alignnone\"><img loading=\"lazy\" decoding=\"async\" aria-describedby=\"caption-attachment-1837\" id=\"Fig3\" class=\"wp-image-1837 size-full\" src=\"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-content\/uploads\/sites\/105\/2016\/08\/EMWave3.png\" alt=\"EMWave3\" width=\"738\" height=\"508\" srcset=\"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-content\/uploads\/sites\/105\/2016\/08\/EMWave3.png 738w, https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-content\/uploads\/sites\/105\/2016\/08\/EMWave3-150x103.png 150w, https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-content\/uploads\/sites\/105\/2016\/08\/EMWave3-300x207.png 300w, https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-content\/uploads\/sites\/105\/2016\/08\/EMWave3-624x430.png 624w\" sizes=\"auto, (max-width: 738px) 100vw, 738px\" \/><p id=\"caption-attachment-1837\" class=\"wp-caption-text\">Figure 3: Yet another electromagnetic wave<\/p><\/div>\n<p>To eliminate this remaining freedom we can specify the behavior of the electric field vector. If the electric field vector stays in a fixed plane as the wave travels (forcing the magnetic field vector to stay in a perpendicular fixed plane) we say that the wave is linearly (or plane) polarized in the direction of the electric field vector.\u00a0 So, the wave in <a href=\"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/lab-3-polarization-of-light\/lab-3-background\/#Fig1\">Fig. 1<\/a> is linearly polarized in the \\(\\hat{y}\\) direction, the wave in <a href=\"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/lab-3-polarization-of-light\/lab-3-background\/#Fig2\">Fig. 2<\/a> is linearly polarized in the \\(\\hat{z}\\) direction, and the wave in <a href=\"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/lab-3-polarization-of-light\/lab-3-background\/#Fig3\">Fig. 3<\/a> is linearly polarized in a direction \\(45^{\\circ}\\) between the two,\u00a0\\(\\frac{1}{\\sqrt{2}}\\left(\\hat{y}+\\hat{z}\\right)\\).<\/p>\n<p>If we add up many waves with random polarizations, so no particular direction of the electric field vector is favored, we have unpolarized light. We will explore how unpolarized light can become polarized, and we will attempt to verify the <a id=\"LawOfMalus\"><\/a>law of Malus which governs the intensity of light transmitted through consecutive ideal <a href=\"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/lab-3-polarization-of-light\/lab-3-equipment\/#Polarizer\">polarizers<\/a> with polarizing directions differing by an angle \\(\\theta\\):<\/p>\n<p>$$I_{\\rm transmitted}=I_{\\rm incident}\\cos^{2}\\theta.$$<\/p>\n<p><a href=\"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/lab-3-polarization-of-light\/lab-3-equipment\/\">Equipment<\/a> <a href=\"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/lab-3-polarization-of-light\/lab-3-data-collection-and-analysis\/\">Data Collection and Analysis<\/a> <a href=\"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/lab-3-polarization-of-light\/lab-3-summary-questions\/\">Summary Questions<\/a><\/p>\n<p><a href=\"http:\/\/www.mathjax.org\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-1256 size-full\" src=\"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-content\/uploads\/sites\/105\/2015\/08\/badge7.gif\" alt=\"badge\" width=\"128\" height=\"37\" \/><\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Suppose that we want to specify the orientation of a plane electromagnetic wave in space (this could be helpful for understanding radio reception, to pick a random example).\u00a0 Plane electromagnetic waves are transverse waves, so we know that the electric and magnetic field vectors are oscillating perpendicularly to the direction of travel, as shown in [&hellip;]<\/p>\n","protected":false},"author":289,"featured_media":0,"parent":1779,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-1781","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-json\/wp\/v2\/pages\/1781","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-json\/wp\/v2\/users\/289"}],"replies":[{"embeddable":true,"href":"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-json\/wp\/v2\/comments?post=1781"}],"version-history":[{"count":0,"href":"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-json\/wp\/v2\/pages\/1781\/revisions"}],"up":[{"embeddable":true,"href":"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-json\/wp\/v2\/pages\/1779"}],"wp:attachment":[{"href":"https:\/\/courses.bowdoin.edu\/physics-1140-lab-manual\/wp-json\/wp\/v2\/media?parent=1781"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}