# The circuit e text main menu textbook table of

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Unformatted text preview: ly made from metallic alloys and carbon compounds. The circuit | e-Text Main Menu | Textbook Table of Contents | Problem Solving Workbook Contents CHAPTER 2 Basic Laws 29 symbol for the resistor is shown in Fig. 2.1(b), where R stands for the resistance of the resistor. The resistor is the simplest passive element. Georg Simon Ohm (1787–1854), a German physicist, is credited with ﬁnding the relationship between current and voltage for a resistor. This relationship is known as Ohm’s law. Ohm’s law states that the voltage v across a resistor is directly proportional to the current i ﬂowing through the resistor. That is, v∝i (2.2) Ohm deﬁned the constant of proportionality for a resistor to be the resistance, R . (The resistance is a material property which can change if the internal or external conditions of the element are altered, e.g., if there are changes in the temperature.) Thus, Eq. (2.2) becomes v = iR (2.3) which is the mathematical form of Ohm’s law. R in Eq. (2.3) is measured in the unit of ohms, designated . Thus, The resistance R of an element denotes its ability to resist the ﬂow of electric current; it is measured in ohms ( ). We may deduce from Eq. (2.3) that R= v i + v=0 R=0 so that 1 − = 1 V/A To apply Ohm’s law as stated in Eq. (2.3), we must pay careful attention to the current direction and voltage polarity. The direction of current i and the polarity of voltage v must conform with the passive sign convention, as shown in Fig. 2.1(b). This implies that current ﬂows from a higher potential to a lower potential in order for v = iR . If current ﬂows from a lower potential to a higher potential, v = −iR . Since the value of R can range from zero to inﬁnity, it is important that we consider the two extreme possible values of R . An element with R = 0 is called a short circuit, as shown in Fig. 2.2(a). For a short circuit, v = iR = 0 v v | e-Text Main Menu | Textbook Table of Contents | (a) + v i=0 R=∞ − (2.5) showing that the voltage is zero but the current could be anything. In practice, a short ci...
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## This note was uploaded on 07/16/2012 for the course KA KA 2000 taught by Professor Bkav during the Spring '12 term at Cambridge.

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