Slide 1Atomic structureCharges in solidsInsulating solidsHow to charge an objectSummaryWhat are we going to learn? A road mapElectric FieldsSuperpositionExampleElectric Field LinesElectric Field of a DipoleElectric Field ON axis of dipoleElectric Field ON axis of dipoleSummaryPhysics 2102 Introduction to Electricity, Magnetism and OpticsPhysics 2102Gabriela GonzálezCharles-Augustin de Coulomb (1736-1806)• negative electron cl oud• nucleus of positive protons, uncharged neutrons• Z = atomic number = # of protons = # of electrons in a neutral atom• A = mass number = # of protons (Z) + # of neutrons (N)• electron charge = e = -1.6 x 10-19 Coulombs = - proton charge• electron mass = 9.10938188 × 10-31 kilograms• proton mass = 1.67262158 × 10-27 kilograms = neutron massAtomic structure•In a conductor, electrons move around freely, forming a “sea” of electrons. This is why metals conduct electricity.•Charges can be “induced” (moved around) in conductors. Charges in solidsBlue background = mobile electronsRed circles = static positive charge (nuclei)--++Insulating solids•In an insulator, each electron cloud is tightly bound to the protons in a nucleus. Wood, glass, rubber.•Note that the electrons are not free to move throughout the lattice, but the electron cloud can “distort” locally.+-How to charge an object•An object can be given some “excess” charge: giving electrons to it (we give it negative charge) or taking electrons away (we “give” it positive charge). •How do we do charge an object? Usually, moving charges from one surface to another by adhesion (helped by friction), or by contact with other charged objects.•If a conductor, the whole electron sea redistributes itself.•If an insulator, the electrons stay where they are put.Summary• Electric charges come with two signs: positive and negative.• Like charges repel, opposite charges attract, with a magnitude calculated from Coulomb’s law: F=kq1q2/r2• Atoms have a positive nucleus and a negative “cloud”.• Electron clouds can combine and flow freely in conductors; are stuck to the nucleus in insulators.•We can charge objects by transferring charge, or by induction.• Electrical charge is conserved, and quantized.What are we going to learn?A road map•Electric charge •Electric force on other electric charges•Electric field, and electric potential•Moving electric charges : current •Electronic circuit components: batteries, resistors, capacitors•Electric currents• Magnetic field •Magnetic force on moving charges•Time-varying magnetic field •Electric Field•More circuit components: inductors •All together: Maxwell’s equations•Electromagnetic waves •Optical images•Matter wavesElectric Fields•Electric field E at some point in space is defined as the force experienced by an i maginary point charge of +1 C, divided by 1 C.•Note that E is a VECTOR.•Since E is the force per unit charge, it is measured in units of N/C. •We measure the electric field using very small “test charges”, and dividing the measured force by the magnitude of the charge. 2||||RqkE +1 CREqElectric field of a point chargeSuperposition•Question: How do we figure out the field due to several point charges?•Answer: consider one charge at a time, calculate the field (a vector!) produced by each charge, and then add all the vectors! (“superposition”)•Useful to look out for SYMMETRY to simplify calculations!Example •4 charges are placed at the corners of a square as shown. •What is the direction of the electric field at the center of the square?(a) Field is zero(b) Along +y(c) Along +x-q-2q+2q+qyxTotal electric fieldElectric Field Lines •Field lines: useful way to visualize electric field E•Field lines start at a positive charge, end at negative charge•E at any point in space is tangential to field line•Field lines are closer where E is strongerExample: a negative point charge -- note spherical symmetryElectric Field of a Dipole •Electric dipole: two point charges +q and -q separated by a distance a•Common arrangement in Nature: molecules, antennae, …•Note axial or cylindrical symmetryPlay hockey with electric charges and learn!http://phet.colorado.edu/en/simulation/electric-hockeyElectric Field ON axis of dipole EEE :ionSuperposit222121axaxkqE22242axxakqPax-q+qax-q+q22axkqE22axkqEElectric Field ON axis of dipole2222224242axkpxaxxakqEWhat if x>> a? (i.e. very far away)p = qa“dipole moment”-- VECTOR - +3422xkpxkpxE 3rpEE~p/r3 is actually true for ANY point far from a dipole (not just on axis)Summary•Electric field is the electric force on an imaginary unit positive charge. •Electric field lines start or end in electric charges.•When fields are strong, electric field lines get closer. •Electric field of a single charge is |E|=kq/r2•The “dipole moment” vector p has magnitude qa and direction from –ve to +ve charge.•Far from a dipole,
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