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B = curl A
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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.
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If there is a particle moving perpendicular to the magnetic field, a force in the direction of the magnetic field is generated.
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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.
- For example, a non-looping line cannot create a magnetic field.
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Intuition:
- Curling current -> straight field
- Straight current -> curling field
- I have this intuition (blu3mo)
- It’s about and .
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The current I/A absorbs the dimension of the length^2 in the volume integral.
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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.
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Ampere’s Law
- curl B = μJ
- It makes sense dimensionally (blu3mo).
- It is important to check how the surface conditions are derived from here.
- curl B = μJ
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Is the Earth a coil because it is a rotating charge?
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.
- 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.