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Electricity and Magnetism
Mathematical Tools and Fields
01Series Approximations: Keeping One or Two Terms02Integrals as Sums: Along a Line and a Curved Path03Line Integrals: Work as the Integral of F · ds04Closed Line Integrals: Work Around a Loop05Double Integrals: Area, Charge and Volume06Closed Surface Integrals: The Sphere and Its Charge07Electric Flux Through Surfaces and Volume IntegralsProblem set0/10Problem set 20/10MIT problem set0/4
01Field Theory Versus Action at a Distance02Scalar Fields: Contour, Color and Relief Maps03Vector Fields, Sources, Sinks and Divergence04Curl: Measuring the Circulation of a Field05Gravitational, Electric and Magnetic Fields06Drawing Vector Fields: Arrows, Lines and Grass SeedsProblem set0/10Problem set 20/10MIT problem set0/1
Electrostatics
01Coulomb's Law: Force Between Two Point Charges02Superposition: Adding Coulomb Forces as Vectors03Field Lines, Null Points and Uniform Fields04The Electric Dipole and Its 1/r³ Field05Torque, Energy and Force on a Dipole in a FieldProblem set0/10Problem set 20/10MIT problem set0/1
01Charge Density and the Field on a Rod's Axis02The Field on a Charged Rod's Perpendicular Bisector03The Fields of a Charged Ring and a Charged Disk04How Field Lines Carry Force, Energy and Momentum05Electric Pressure and Tension: The Stress ε₀E²/2Problem set0/10Problem set 20/10MIT problem set0/6

How Field Lines Carry Force, Energy and Momentum

If there is no action at a distance, how do field lines carry force, energy and momentum between charges?


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Your summary note

    1. 1

      Repulsion and attraction near a van de Graaff sphere

      Sketch the total field lines for a small sphere carrying like and then unlike charge, and state that the force passes through the field at the speed of light, not by action at a distance.

    2. 2

      Tension and pressure giving the force qE⃗q\vec{E}qE

      Draw the charge at rest at the origin in E⃗=−E0k^\vec{E} = -E_0\hat{\mathbf{k}}E=−E0​k^ with an imaginary sphere around it, mark where the lines pull and where they push, and show both give −qE0k^-qE_0\hat{\mathbf{k}}−qE0​k^.

    3. 3

      Energy and momentum exchanged with the field

      Trace the charge rising, stopping and falling back, record where its kinetic energy goes as it slows and where it comes from as it speeds up, and state which objects receive its zzz-momentum.

    Attempt 1 of 2