{"id":890,"date":"2019-07-26T18:48:52","date_gmt":"2019-07-26T18:48:52","guid":{"rendered":"https:\/\/pressbooks.bccampus.ca\/physics216\/chapter\/introduction-15\/"},"modified":"2021-09-16T12:12:00","modified_gmt":"2021-09-16T12:12:00","slug":"introduction-15","status":"publish","type":"chapter","link":"https:\/\/pressbooks.bccampus.ca\/physics216\/chapter\/introduction-15\/","title":{"raw":"15 Introduction","rendered":"15 Introduction"},"content":{"raw":"
\r\n\r\n[caption id=\"\" align=\"aligncenter\" width=\"975\"]\"Photograph Figure 15.1<\/strong> The current we draw into our houses is an alternating current (ac). Power lines transmit ac to our neighborhoods, where local power stations and transformers distribute it to our homes. In this chapter, we discuss how a transformer works and how it allows us to transmit power at very high voltages and minimal heating losses across the lines.[\/caption]\r\n\r\n<\/div>\r\n

Chapter Outline<\/h2>\r\n
15.1<\/span>\u00a0AC Sources<\/span><\/a><\/div>\r\n
15.2<\/span>\u00a0Simple AC Circuits<\/span><\/a><\/div>\r\n
15.3<\/span>\u00a0RLC Series Circuits with AC<\/span><\/a><\/div>\r\n
15.4<\/span>\u00a0Power in an AC Circuit<\/span><\/a><\/div>\r\n
15.5<\/span>\u00a0Resonance in an AC Circuit<\/span><\/a><\/div>\r\n
15.6<\/span>\u00a0Transformers<\/span><\/a><\/div>\r\n

Electric power is delivered to our homes by alternating current (ac) through high-voltage transmission lines. As explained in Transformers<\/a>, transformers can then change the amplitude of the alternating potential difference to a more useful form. This lets us transmit power at very high voltages, minimizing resistive heating losses in the lines, and then furnish that power to homes at lower, safer voltages. Because constant potential differences are unaffected by transformers, this capability is more difficult to achieve with direct-current transmission.<\/p>\r\n

In this chapter, we use Kirchhoff\u2019s laws to analyze four simple circuits in which ac flows. We have discussed the use of the resistor, capacitor, and inductor in circuits with batteries. These components are also part of ac circuits. However, because ac is required, the constant source of emf supplied by a battery is replaced by an ac voltage source, which produces an oscillating emf.<\/p>","rendered":"

\n
\"Photograph
Figure 15.1<\/strong> The current we draw into our houses is an alternating current (ac). Power lines transmit ac to our neighborhoods, where local power stations and transformers distribute it to our homes. In this chapter, we discuss how a transformer works and how it allows us to transmit power at very high voltages and minimal heating losses across the lines.<\/figcaption><\/figure>\n<\/div>\n

Chapter Outline<\/h2>\n
15.1<\/span>\u00a0AC Sources<\/span><\/a><\/div>\n
15.2<\/span>\u00a0Simple AC Circuits<\/span><\/a><\/div>\n
15.3<\/span>\u00a0RLC Series Circuits with AC<\/span><\/a><\/div>\n
15.4<\/span>\u00a0Power in an AC Circuit<\/span><\/a><\/div>\n
15.5<\/span>\u00a0Resonance in an AC Circuit<\/span><\/a><\/div>\n
15.6<\/span>\u00a0Transformers<\/span><\/a><\/div>\n

Electric power is delivered to our homes by alternating current (ac) through high-voltage transmission lines. As explained in Transformers<\/a>, transformers can then change the amplitude of the alternating potential difference to a more useful form. This lets us transmit power at very high voltages, minimizing resistive heating losses in the lines, and then furnish that power to homes at lower, safer voltages. Because constant potential differences are unaffected by transformers, this capability is more difficult to achieve with direct-current transmission.<\/p>\n

In this chapter, we use Kirchhoff\u2019s laws to analyze four simple circuits in which ac flows. We have discussed the use of the resistor, capacitor, and inductor in circuits with batteries. These components are also part of ac circuits. However, because ac is required, the constant source of emf supplied by a battery is replaced by an ac voltage source, which produces an oscillating emf.<\/p>\n","protected":false},"author":65,"menu_order":1,"template":"","meta":{"pb_show_title":"on","pb_short_title":"","pb_subtitle":"","pb_authors":[],"pb_section_license":""},"chapter-type":[48],"contributor":[],"license":[],"class_list":["post-890","chapter","type-chapter","status-publish","hentry","chapter-type-numberless"],"part":888,"_links":{"self":[{"href":"https:\/\/pressbooks.bccampus.ca\/physics216\/wp-json\/pressbooks\/v2\/chapters\/890","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/pressbooks.bccampus.ca\/physics216\/wp-json\/pressbooks\/v2\/chapters"}],"about":[{"href":"https:\/\/pressbooks.bccampus.ca\/physics216\/wp-json\/wp\/v2\/types\/chapter"}],"author":[{"embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/physics216\/wp-json\/wp\/v2\/users\/65"}],"version-history":[{"count":4,"href":"https:\/\/pressbooks.bccampus.ca\/physics216\/wp-json\/pressbooks\/v2\/chapters\/890\/revisions"}],"predecessor-version":[{"id":1184,"href":"https:\/\/pressbooks.bccampus.ca\/physics216\/wp-json\/pressbooks\/v2\/chapters\/890\/revisions\/1184"}],"part":[{"href":"https:\/\/pressbooks.bccampus.ca\/physics216\/wp-json\/pressbooks\/v2\/parts\/888"}],"metadata":[{"href":"https:\/\/pressbooks.bccampus.ca\/physics216\/wp-json\/pressbooks\/v2\/chapters\/890\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/pressbooks.bccampus.ca\/physics216\/wp-json\/wp\/v2\/media?parent=890"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/physics216\/wp-json\/pressbooks\/v2\/chapter-type?post=890"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/physics216\/wp-json\/wp\/v2\/contributor?post=890"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/physics216\/wp-json\/wp\/v2\/license?post=890"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}