The closed loop line integral of a magnetic field is proportional to the current the loop encloses. Right hand rule dictates the sign of the integral. Over a stationary path.
It is an incomplete model without Ampère’s Law With Maxwell’s Addition
The closed loop line integral of a magnetic field is proportional to the current the loop encloses. Right hand rule dictates the sign of the integral. Over a stationary path.
It is an incomplete model without Ampère’s Law With Maxwell’s Addition