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© 2014 Pearson Education, Inc. This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their courses and assessing student learning. Dissemination or sale of any part of this work (including on the World Wide Web) will destroy the integrity of the work and is not permitted. The work and materials from it should never be made available to students except by instructors using the accompanying text in their classes. All recipients of this work are expected to abide by these restrictions and to honor the intended pedagogical purposes and the needs of other instructors who rely on these materials. Lecture PowerPoints Chapter 18 Physics: Principles with Applications, 7 th edition Giancoli

Chapter 18 Electric Currents © 2014 Pearson Education, Inc.

Contents of Chapter 18 The Electric Battery Electric Current Resistivity Ohm’s Law: Resistance and Resistors Electric Power © 2014 Pearson Education, Inc.

18-1 EMF and Terminal Voltage Volta discovered that electricity could be created if dissimilar metals were connected by a conductive solution called an electrolyte. This is a simple electric cell. © 2014 Pearson Education, Inc.

18-1 EMF and Terminal Voltage Electric circuit needs battery or generator to produce current—these are called sources of emf. Battery is a nearly constant voltage source, but does have a small internal resistance, which reduces the actual voltage from the ideal emf: © 2014 Pearson Education, Inc. (19-1)

18-1 EMF and Terminal Voltage A battery transforms chemical energy into electrical energy. Chemical reactions within the cell create a potential difference between the terminals by slowly dissolving them. This potential difference can be maintained even if a current is kept flowing, until one or the other terminal is completely dissolved. © 2014 Pearson Education, Inc.

18-1 EMF and Terminal Voltage Several cells connected together make a battery, although now we refer to a single cell as a battery as well. © 2014 Pearson Education, Inc.

18-1 EMF and Terminal Voltage This resistance behaves as though it were in series with the emf. © 2014 Pearson Education, Inc.

18-2 Electric Current Electric current is the rate of flow of charge through a conductor: Unit of electric current: the ampere, A. 1 A = 1 C/s © 2014 Pearson Education, Inc. (18-1)

18-2 Electric Current A complete circuit is one where current can flow all the way around. Note that the schematic drawing doesn’t look much like the physical circuit! © 2014 Pearson Education, Inc.

18-2 Electric Current In order for current to flow, there must be a path from one battery terminal, through the circuit, and back to the other battery terminal. Only one of these circuits will work: © 2014 Pearson Education, Inc.

18-2 Electric Current By convention, current is defined as flowing from + to –. Electrons actually flow in the opposite direction, but not all currents consist of electrons. © 2014 Pearson Education, Inc.

18-3 Resistivity The resistance of a wire is directly proportional to its length and inversely proportional to its cross-sectional area: The constant ρ, the resistivity, is characteristic of the material. © 2014 Pearson Education, Inc. (18-3)

18-3 Resistivity © 2014 Pearson Education, Inc.

18-4 Ohm’s Law: Resistance and Resistors Experimentally, it is found that the current in a wire is proportional to the potential difference between its ends: I  V © 2014 Pearson Education, Inc.

18-4 Ohm’s Law: Resistance and Resistors The ratio of voltage to current is called the resistance: © 2014 Pearson Education, Inc. (18-2)

18-4 Ohm’s Law: Resistance and Resistors In many conductors, the resistance is independent of the voltage; this relationship is called Ohm’s law. Materials that do not follow Ohm’s law are called nonohmic. Unit of resistance: the ohm, Ω. 1 Ω = 1 V/A © 2014 Pearson Education, Inc.

18-4 Ohm’s Law: Resistance and Resistors Some clarifications: Batteries maintain a (nearly) constant potential difference; the current varies. Resistance is a property of a material or device. Current is not a vector but it does have a direction. Current and charge do not get used up. Whatever charge goes in one end of a circuit comes out the other end. © 2014 Pearson Education, Inc.

18-5 Electric Power Power, as in kinematics, is the energy transformed by a device per unit time: © 2014 Pearson Education, Inc. (18-5)

18-5 Electric Power The unit of power is the watt, W. For ohmic devices, we can make the substitutions: © 2014 Pearson Education, Inc. (18-6a) (18-6b)

Summary of Chapter 18 A battery is a source of constant potential difference. Electric current is the rate of flow of electric charge. Conventional current is in the direction that positive charge would flow. Resistance is determined by shape and material: ρ is the resistivity. Resistance is the ratio of voltage to current: © 2014 Pearson Education, Inc.

Summary of Chapter 18 Ohmic materials have constant resistance, independent of voltage. Power in an electric circuit: © 2014 Pearson Education, Inc.