• B = curl A

  • div B = 0

    • This is obvious considering that there is no magnetic charge and Gauss’s law.
    • It also matches with div curl A = 0. image
  • If there is a particle moving perpendicular to the magnetic field, a force in the direction of the magnetic field is generated.

  • Charge conservation imposes a strong constraint on the current density, j.

    • For example, a non-looping line cannot create a magnetic field.
      • Because charge cannot continue to move without a loop.
  • Intuition:

    • Curling current -> straight field
    • Straight current -> curling field
    • I have this intuition (blu3mo)
      • It’s about and .
  • The current I/A absorbs the dimension of the length^2 in the volume integral.

  • Equipotential curves have the same shape for both A and Φ.

    • Equipotential curves have the same direction as the vector A.
    • A and B are perpendicular.
  • Ampere’s Law

    • curl B = μJ
      • It makes sense dimensionally (blu3mo).
    • It is important to check how the surface conditions are derived from here.
  • Is the Earth a coil because it is a rotating charge? image

Two wires are approaching.

Integrating (ρ, J) gives (σ, κ).

  • In SI units, there is a dimensional difference between the magnetic field and the electric field due to c. image
  • This is the contribution of the cross term (B_y contributes to E_x).

Just like the electric field, the perpendicular component of the B field does not change under a boost.

  • There is a variant of the cross product between a vector and a boost that resembles LT.