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:<math>\mathfrak{r}\ \stackrel{def}{=}\ \frac{\mathrm{d}V}{\mathrm{d}I}</math>, |
:<math>\mathfrak{r}\ \stackrel{def}{=}\ \frac{\mathrm{d}V}{\mathrm{d}I}</math>, |
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此動態的電阻量適用於計算非歐姆元件,動態電阻的單位一樣也是[[歐姆]]<ref name=horowitz-hill>{{cite book |last=Horowitz |first=Paul|coauthors=Winfield Hill| title=The Art of Electronics | |
此動態的電阻量適用於計算非歐姆元件,動態電阻的單位一樣也是[[歐姆]]<ref name=horowitz-hill>{{cite book |last=Horowitz |first=Paul|coauthors=Winfield Hill| title=The Art of Electronics ||edition=2nd |year=1989 |publisher=Cambridge University Press |isbn=0-521-37095-7 |page = [https://archive.org/details/artelectronics00horo/page/n31 13] }}</ref>。 |
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== 溫度對電阻的影響 == |
== 溫度對電阻的影響 == |
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=== 導電體 === |
=== 導電體 === |
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[[File:TCR_Copper.png|缩略图|250px|[[銅]]金屬在不同溫度狀況的電阻溫度係數<ref name=handbook>{{Citation | editor = Pender, Harold & Del Mar, William | title = Handbook for Electrical Engineers:a reference book for practicing engineers and students | place = New York | publisher = John Wiley & Sons, Inc. | year = 1922 | edition = 2nd | pages =pp. 1350, 2094 | |
[[File:TCR_Copper.png|缩略图|250px|[[銅]]金屬在不同溫度狀況的電阻溫度係數<ref name=handbook>{{Citation | editor = Pender, Harold & Del Mar, William | title = Handbook for Electrical Engineers:a reference book for practicing engineers and students | place = New York | publisher = John Wiley & Sons, Inc. | year = 1922 | edition = 2nd | pages =pp. 1350, 2094 | |
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}}</ref>。]] |
}}</ref>。]] |
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假設[[溫度]]接近[[室溫]],則典型金屬的電阻<math>R</math>通常與溫度<math>T</math>成[[正比]]<ref>{{Citation | last = Bird | first = John | title = Electrical and electronic principles and technology | publisher = Newnes | year = 2006 | pages = pp. 22-24 | isbn = 9780750685566}}</ref>: |
假設[[溫度]]接近[[室溫]],則典型金屬的電阻<math>R</math>通常與溫度<math>T</math>成[[正比]]<ref>{{Citation | last = Bird | first = John | title = Electrical and electronic principles and technology | publisher = Newnes | year = 2006 | pages = pp. 22-24 | isbn = 9780750685566}}</ref>: |
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其中,<math>C_l</math>是比例常數。 |
其中,<math>C_l</math>是比例常數。 |
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[[File:Electrical Resistance Vs Temperature.png|缩略图|200px|[[水銀]]、[[白金]]、[[黃金]]在不同溫度狀況的電阻<ref>{{Citation | last = 昂內斯 | first = 海克 | |
[[File:Electrical Resistance Vs Temperature.png|缩略图|200px|[[水銀]]、[[白金]]、[[黃金]]在不同溫度狀況的電阻<ref>{{Citation | last = 昂內斯 | first = 海克 | | title = Investigations into the properties of substances at low temperatures, which have led, amongst other things, to the preparation of liquid helium. | publisher = Nobel Lecture | url = http://nobelprize.org/physics/laureates/1913/onnes-lecture.pdf | date = 1913年12月 | accessdate = 2010-12-23 | | | }}</ref>。]] |
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如右圖所示,當溫度接近[[絕對溫度]]時,[[黃金]]和[[白金]]的電阻趨向於常數;而當溫度小於4.2K時,[[水銀]]的電阻突然從0.002歐姆陡降為10<sup>−6</sup>歐姆,成為[[超導體]]。 |
如右圖所示,當溫度接近[[絕對溫度]]時,[[黃金]]和[[白金]]的電阻趨向於常數;而當溫度小於4.2K時,[[水銀]]的電阻突然從0.002歐姆陡降為10<sup>−6</sup>歐姆,成為[[超導體]]。 |
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== 外部連結 == |
== 外部連結 == |
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* 克萊門森大學車輛電子實驗室網頁:[ |
* 克萊門森大學車輛電子實驗室網頁:[http://www.cvel.clemson.edu/emc/calculators/Resistance_Calculator/index.html 電阻計算機]{{en}} |
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{{电磁学}} |
{{电磁学}} |