{"id":2390,"date":"2023-12-11T05:35:28","date_gmt":"2023-12-10T22:35:28","guid":{"rendered":"https:\/\/www.tneutron.net\/elektro\/?p=2390"},"modified":"2023-12-08T19:13:18","modified_gmt":"2023-12-08T12:13:18","slug":"strength-lorentz","status":"publish","type":"post","link":"https:\/\/www.tneutron.net\/elektro\/strength-lorentz\/","title":{"rendered":"Strength Lorentz"},"content":{"rendered":"<p><span class=\"notranslate\">Lorentz force strength will be influenced by factors in the formula above.<\/span> <span class=\"notranslate\"> If a conductor in a magnetic field in amounts greater than one, then the strength of the Lorentz force will be proportional to the number of conductors.<\/span> <span class=\"notranslate\"> So the formula above multiplied by the number of conductors.<\/span><\/p>\n<p><span class=\"notranslate\"> <strong>The coils have current in a Magnetic Field<\/strong><\/span> <strong><br \/>\n<\/strong> <span class=\"notranslate\"> The coil when placed in a magnetic field, then the coil will rotate.<\/span><br \/>\n<a href=\"https:\/\/www.tneutron.net\/elektro\/wp-content\/uploads\/sites\/2\/2016\/11\/image-28.png\"><img loading=\"lazy\" decoding=\"async\" title=\"image\" src=\"https:\/\/www.tneutron.net\/elektro\/wp-content\/uploads\/sites\/2\/2016\/11\/image_thumb-28.png\" alt=\"image\" width=\"320\" height=\"171\" border=\"0\" \/><\/a><br \/>\n<span class=\"notranslate\"> Pictures 1132 (a) Directions terrain surrounding the conductor in the coil and (b) the magnetic field direction.<\/span><\/p>\n<p><span class=\"notranslate\">The cross-section cut from a coil depicted with two conductors with the opposite direction of the current.<\/span> <span class=\"notranslate\"> In Figure 1.132a shown, marked with a cross sectional top being the bottom of the home point.<\/span> <span class=\"notranslate\"> Terrain around the conductor as shown in Figure 1.132a.<\/span> <span class=\"notranslate\"> When the current carrying coil placed in a magnetic field it will be visible in the 1133 image.<\/span> <span class=\"notranslate\"> On the sides of the conductor will be weakening and strengthening of the field depending on the direction of the field around the conductor with the magnetic field of the magnet poles.<\/span><br \/>\n<a href=\"https:\/\/www.tneutron.net\/elektro\/wp-content\/uploads\/sites\/2\/2016\/11\/image-29.png\"><img loading=\"lazy\" decoding=\"async\" title=\"image\" src=\"https:\/\/www.tneutron.net\/elektro\/wp-content\/uploads\/sites\/2\/2016\/11\/image_thumb-29.png\" alt=\"image\" width=\"278\" height=\"196\" border=\"0\" \/><\/a><br \/>\n<span class=\"notranslate\"> Image 1133 Directions motion coil in a magnetic field.<\/span><\/p>\n<p><span class=\"notranslate\"> As a result, the upper conductor will move to the left and below the conductors will move to the right.<\/span> <span class=\"notranslate\"> This is in accordance with the rules of his left hand.<\/span> <span class=\"notranslate\"> When the coil has transverse 90 <sup>0<\/sup> to the magnetic field, then the coil will stop moving.<\/span> <span class=\"notranslate\"> As shown in Figure 1.134 below.<\/span><br \/>\n<a href=\"https:\/\/www.tneutron.net\/elektro\/wp-content\/uploads\/sites\/2\/2016\/11\/image-30.png\"><img loading=\"lazy\" decoding=\"async\" title=\"image\" src=\"https:\/\/www.tneutron.net\/elektro\/wp-content\/uploads\/sites\/2\/2016\/11\/image_thumb-30.png\" alt=\"image\" width=\"299\" height=\"185\" border=\"0\" \/><\/a><br \/>\n<span class=\"notranslate\"> Image 1134 Directions motion when the coil 90 <sup>0<\/sup> to the magnetic field.<\/span><\/p>\n<p><span class=\"notranslate\">Torque from the coil can be calculated with the following formula:<\/span><br \/>\n<a href=\"https:\/\/www.tneutron.net\/elektro\/wp-content\/uploads\/sites\/2\/2016\/11\/image-31.png\"><img loading=\"lazy\" decoding=\"async\" title=\"image\" src=\"https:\/\/www.tneutron.net\/elektro\/wp-content\/uploads\/sites\/2\/2016\/11\/image_thumb-31.png\" alt=\"image\" width=\"125\" height=\"88\" border=\"0\" \/><\/a><br \/>\n<span class=\"notranslate\"> M = torque<\/span><br \/>\n<span class=\"notranslate\"> Lorentz force F = one conductor<\/span><br \/>\n<span class=\"notranslate\"> r = radius of coil<\/span><br \/>\n<span class=\"notranslate\"> d = diameter of the coil<\/span><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Lorentz force strength will be influenced by factors in the formula above. If a conductor in a magnetic field in<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"colormag_page_container_layout":"default_layout","colormag_page_sidebar_layout":"default_layout","footnotes":""},"categories":[2232],"tags":[2902,2903,2905,2911,2907,2908,2906,2904,2910,2909],"class_list":["post-2390","post","type-post","status-publish","format-standard","hentry","category-english","tag-magnetic-field","tag-magnetic-field-definition","tag-magnetic-field-equation","tag-magnetic-field-formula","tag-magnetic-field-lines","tag-magnetic-field-of-earth","tag-magnetic-field-strength","tag-magnetic-fields-band","tag-magnetic-fields-mass-moca","tag-magnetic-fields-tour"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.9 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>Strength Lorentz - TN Elektro<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/www.tneutron.net\/elektro\/strength-lorentz\/\" \/>\n<meta name=\"twitter:card\" content=\"summary_large_image\" \/>\n<meta name=\"twitter:title\" content=\"Strength Lorentz - TN Elektro\" \/>\n<meta name=\"twitter:description\" content=\"Lorentz force strength will be influenced by factors in the formula above. 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