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III. Voltage Dr. Bill Pezzaglia Updated 2012Aug06
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A. Voltage 1)Electrostatic Energy 2)Electric Potential (Voltage) 3)Capacitance 2
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1. Electrostatic Potential Energy a)Review Gravitational Potential Energy b)Electrostatic Potential 3
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a) Review: Gravitational Potential Energy Near surface of earth, where gravitational field is constant g=9.8 m/s 2, then the change of potential energy of lifting a mass “m” up a distance “h” is just: U=mgh For large distances, gravity follows the inverse square law. A body “m” falling from infinity to the surface of the earth (mass “M”) will have a change of potential energy of: This would be the amount of energy that a meteor would have hitting the earth and making a big crater! 4
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b) Electrostatic Potential Energy Electric fields also follow the inverse square law. Hence a small test charge “q” pushed from infinity onto a massive ball of charge “Q” of radius “R” will have a change of potential energy of: 5 Note: energy of two positive (or two negative) charges is positive Energy of positive and negative charge is negative
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2. Voltage a)Definition of Voltage b)Sources of Voltage c)Measuring Voltage 6
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2a. Definition of voltage Potential Energy per unit test charge: (i.e. don’t want test charge to affect field) Units: Volt=Joule/Coulomb Voltage is the “pressure” that makes charges move (current flow). Even if there is no test charge to experience it, voltage exists 7
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2ai. Cathode Ray Tube A CRT (Cathode Ray Tube) is a vacuum tube with a large voltage across the electrodes. Electrons are emitted by the Cathode and accelerate towards the anode. Kinetic energy the electrons gain is hence: U=e V 1 eV = 1 electron volt is the energy of one electron accelerated through one volt = 1.6x10 -19 Joules. 8 http://www.youtube.com/v/XU8nMKkzbT8?f=videos&app=youtube_gdata&autoplay=1
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2aii. Particle Accelerators SLAC (Stanford Linear Accelerator Center) accelerates electrons to 50 GeV of energy Note: the E=mc 2 rest-mass energy of a proton is only 938 MeV 9
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2b. Sources of Voltage (a)Point Charge Source (b)Superposition of Point Charges (c)Batteries (d)Thermo and Piezoelectrics 10
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2bi. Charge as Source of Voltage Define the voltage at infinity to be zero Voltage a distance “r” from the center of a spherical charge Q is: 11
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2bii. Batteries are a source of voltage Volta (1745-1827) “The Newton of electricity” 1800 develops first battery (approximately 30 volts) By adding batteries together in series, one can make as big as voltage as you want. 12 http://www.corrosion-doctors.org/Biographies/VoltaBio.htm
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2biii. Piezoelectrics etc Some devices that are useful as detectors Thermoelectrics: some materials will create a voltage across them due to a temperature difference Pyroelectrics: heating some materials will create a voltage across them Piezoelectrics: 1880 Pierre Curie demonstrates effect that some crystals generate a voltage when deformed 13
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2c. Measuring Voltage Put a “voltmeter” in parallel with element you wish to measure potential difference 14
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2cii. Oscilloscope Oscilloscopes are used to measure voltage (especially of AC signals). They are essentially a CRT tube with deflection plates. The amount of deflection of the beam is proportional to the voltage across the plates. 15
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