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Published byGabriel Norton Modified over 8 years ago
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Chapter 4 Overview
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Maxwell’s Equations
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Charge Distributions Volume charge density: Total Charge in a Volume Surface and Line Charge Densities
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Current Density For a surface with any orientation: J is called the current density
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Convection vs. Conduction
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Coulomb’s Law Electric field at point P due to single charge Electric force on a test charge placed at P Electric flux density D
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Electric Field Due to 2 Charges
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Electric Field due to Multiple Charges
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Electric Field Due to Charge Distributions Field due to:
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Cont.
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Example 4-5 cont.
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Gauss’s Law Application of the divergence theorem gives:
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Applying Gauss’s Law Construct an imaginary Gaussian cylinder of radius r and height h:
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Electric Scalar Potential Minimum force needed to move charge against E field:
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Electric Scalar Potential
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Electric Potential Due to Charges In electric circuits, we usually select a convenient node that we call ground and assign it zero reference voltage. In free space and material media, we choose infinity as reference with V = 0. Hence, at a point P For a point charge, V at range R is: For continuous charge distributions:
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Relating E to V
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Cont.
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(cont.)
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Poisson’s & Laplace’s Equations In the absence of charges:
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Conduction Current Conduction current density: Note how wide the range is, over 24 orders of magnitude
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Conductivity ve = volume charge density of electrons vh = volume charge density of holes e = electron mobility h = hole mobility N e = number of electrons per unit volume N h = number of holes per unit volume
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Resistance For any conductor: Longitudinal Resistor
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G’=0 if the insulating material is air or a perfect dielectric with zero conductivity.
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Joule’s Law The power dissipated in a volume containing electric field E and current density J is: For a resistor, Joule’s law reduces to: For a coaxial cable:
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Wheatstone Bridge Wheatstone bridge is a high sensitivity circuit for measuring small changes in resistance
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Dielectric Materials
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Polarization Field P = electric flux density induced by E
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Electric Breakdown
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Boundary Conditions
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Summary of Boundary Conditions Remember E = 0 in a good conductor
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Conductors Net electric field inside a conductor is zero
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Field Lines at Conductor Boundary At conductor boundary, E field direction is always perpendicular to conductor surface
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Capacitance
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For any two-conductor configuration: For any resistor:
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Application of Gauss’s law gives: Q is total charge on inside of outer cylinder, and –Q is on outside surface of inner cylinder
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Electrostatic Potential Energy Electrostatic potential energy density (Joules/volume) Total electrostatic energy stored in a volume Energy stored in a capacitor
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Image Method Image method simplifies calculation for E and V due to charges near conducting planes. 1.For each charge Q, add an image charge –Q 2.Remove conducting plane 3.Calculate field due to all charges
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