Ludium
Sign In
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

Field Lines, Null Points and Uniform Fields

Where does the field of two charges vanish, and what do field lines reveal about charges and uniform fields?


Loading…

←Previous Superposition: Adding Coulomb Forces as VectorsNext The Electric Dipole and Its 1/r³ Field →

Your summary note

    1. 1

      The electric field E⃗=lim⁡q0→0F⃗e/q0\vec{E} = \lim_{q_0 \to 0} \vec{F}_e/q_0E=limq0​→0​Fe​/q0​

      Write the test-charge definition beside its gravitational analogue g⃗\vec{g}g​, combine it with Coulomb's law to get the point-charge field, add the sum E⃗=∑iE⃗i\vec{E} = \sum_i \vec{E}_iE=∑i​Ei​, and record F⃗e=q0E⃗\vec{F}_e = q_0\vec{E}Fe​=q0​E.

    2. 2

      Field-line pattern of a charge pair from four considerations

      Sketch the field lines of a charge pair and annotate how symmetry, the near field, the far field of Q=∑iQiQ = \sum_i Q_iQ=∑i​Qi​, and null points where E⃗=0⃗\vec{E} = \vec{0}E=0 each shape the picture.

    3. 3

      The four properties of field lines

      List them: E⃗\vec{E}E tangent to the line, lines starting on positive and ending on negative charges or at infinity, line count proportional to charge, and no two lines crossing.

    4. 4

      Charge released from rest between parallel plates

      Derive a⃗=qE⃗/m\vec{a} = q\vec{E}/ma=qE/m, v=2yqEy/mv = \sqrt{2yqE_y/m}v=2yqEy​/m​ and K=qEyyK = qE_y yK=qEy​y with units checked, and record that the kinetic energy comes from the field while the momentum comes from the source charges.

    Attempt 1 of 2