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-- card: 3405 from stack: in -- bmap block id: 5985 -- flags: 0000 -- background id: 3771 -- name: -- part 1 (field) -- low flags: 00 -- high flags: 0000 -- rect: left=438 top=123 right=144 bottom=464 -- title width / last selected line: 0 -- icon id / first selected line: 0 / 0 -- text alignment: 0 -- font id: 34 -- text size: 14 -- style flags: 0 -- line height: 18 -- part name: -- part 2 (field) -- low flags: 00 -- high flags: 0000 -- rect: left=417 top=218 right=239 bottom=443 -- title width / last selected line: 0 -- icon id / first selected line: 0 / 0 -- text alignment: 0 -- font id: 34 -- text size: 14 -- style flags: 0 -- line height: 18 -- part name: -- part contents for background part 3 ----- text ----- In Electromagnetic Fields I we will be interested only in static and quasistatic fields. This means that we assume that the time derivatives in Ampere’s Law and Faraday’s Law are small enough that they are not important. These laws now become -- part contents for card part 1 ----- text ----- =0 -- part contents for card part 2 ----- text ----- =0