Chapter 15First Observations – GreeksBenjamin FranklinProperties of Electric ChargesMore Properties of ChargeProperties of Charge, finalConductorsInsulatorsSemiconductorsCharging by ConductionCharging by InductionCharging by Induction, 2Charging by Induction, 3Charging by Induction, finalPolarizationExamples of PolarizationCoulomb’s LawCoulomb’s Law, cont.Characteristics of ParticlesCharles CoulombVector Nature of Electric ForcesVector Nature of Forces, cont.Electrical Forces are Field ForcesElectrical Force Compared to Gravitational ForceThe Superposition PrincipleSuperposition Principle ExampleElectrical FieldElectric Field, cont.Electric FieldDirection of Electric FieldDirection of Electric Field, contMore About a Test Charge and The Electric FieldProblem Solving StrategyProblem Solving Strategy, contProblem Solving Strategy, Electric FieldsElectric Field LinesElectric Field Lines, cont.Electric Field Line PatternsSlide 39Slide 40Slide 41Electric Field PatternsRules for Drawing Electric Field LinesConductors in Electrostatic EquilibriumProperty 1Property 2Property 3Property 4Property 4, cont.Experiments to Verify Properties of ChargesVan de Graaff GeneratorElectric FluxElectric Flux, cont.Gauss’ LawElectric Field of a Charged Thin Spherical ShellElectric Field of a Nonconducting Plane Sheet of ChargeElectric Field of a Nonconducting Plane Sheet of Charge, cont.Parallel Plate CapacitorChapter 15Electric Forces andElectric FieldsFirst Observations – Greeks Observed electric and magnetic phenomena as early as 700 BCFound that amber, when rubbed, became electrified and attracted pieces of straw or feathersAlso discovered magnetic forces by observing magnetite attracting ironBenjamin Franklin1706 – 1790Printer, author, founding father, inventor, diplomatPhysical Scientist1740’s work on electricity changed unrelated observations into coherent scienceProperties of Electric ChargesTwo types of charges existThey are called positive and negativeNamed by Benjamin FranklinLike charges repel and unlike charges attract one anotherNature’s basic carrier of positive charge is the protonProtons do not move from one material to another because they are held firmly in the nucleusMore Properties of ChargeNature’s basic carrier of negative charge is the electronGaining or losing electrons is how an object becomes chargedElectric charge is always conservedCharge is not created, only exchangedObjects become charged because negative charge is transferred from one object to anotherProperties of Charge, finalCharge is quantizedAll charge is a multiple of a fundamental unit of charge, symbolized by eQuarks are the exceptionElectrons have a charge of –eProtons have a charge of +eThe SI unit of charge is the Coulomb (C)e = 1.6 x 10-19 CConductorsConductors are materials in which the electric charges move freely in response to an electric forceCopper, aluminum and silver are good conductorsWhen a conductor is charged in a small region, the charge readily distributes itself over the entire surface of the materialInsulatorsInsulators are materials in which electric charges do not move freelyGlass and rubber are examples of insulatorsWhen insulators are charged by rubbing, only the rubbed area becomes chargedThere is no tendency for the charge to move into other regions of the materialSemiconductorsThe characteristics of semiconductors are between those of insulators and conductorsSilicon and germanium are examples of semiconductorsCharging by ConductionA charged object (the rod) is placed in contact with another object (the sphere)Some electrons on the rod can move to the sphereWhen the rod is removed, the sphere is left with a chargeThe object being charged is always left with a charge having the same sign as the object doing the chargingCharging by InductionWhen an object is connected to a conducting wire or pipe buried in the earth, it is said to be groundedA negatively charged rubber rod is brought near an uncharged sphereCharging by Induction, 2The charges in the sphere are redistributedSome of the electrons in the sphere are repelled from the electrons in the rodCharging by Induction, 3The region of the sphere nearest the negatively charged rod has an excess of positive charge because of the migration of electrons away from this locationA grounded conducting wire is connected to the sphereAllows some of the electrons to move from the sphere to the groundCharging by Induction, finalThe wire to ground is removed, the sphere is left with an excess of induced positive chargeThe positive charge on the sphere is evenly distributed due to the repulsion between the positive chargesCharging by induction requires no contact with the object inducing the chargePolarizationIn most neutral atoms or molecules, the center of positive charge coincides with the center of negative chargeIn the presence of a charged object, these centers may separate slightlyThis results in more positive charge on one side of the molecule than on the other sideThis realignment of charge on the surface of an insulator is known as polarizationExamples of PolarizationThe charged object (on the left) induces charge on the surface of the insulatorA charged comb attracts bits of paper due to polarization of the paperCoulomb’s LawCoulomb shows that an electrical force has the following properties:It is along the line joining the two particles and inversely proportional to the square of the separation distance, r, between them It is proportional to the product of the magnitudes of the charges, |q1|and |q2|on the two particlesIt is attractive if the charges are of opposite signs and repulsive if the charges have the same signsCoulomb’s Law, cont.Mathematically,ke is called the Coulomb Constantke = 8.9875 x 109 N m2/C2Typical charges can be in the µC rangeRemember, Coulombs must be used in the equationRemember that force is a vector quantityApplies only to point charges221erqqkF Characteristics of ParticlesCharles Coulomb1736 – 1806Studied electrostatics and magnetismInvestigated strengths of materialsIdentified forces acting on beamsVector Nature of Electric ForcesTwo point charges are separated by a distance rThe like charges produce a repulsive force between themThe force on q1 is equal in magnitude
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