Electromagnetism – Reasons for the Finite Number of Magnetic Field Lines in a Given Area

electromagnetismintegrationmagnetic fieldsterminologyVector Fields

One can draw/imagine as many unique (curved/straight) lines as he/she wants in some specified finite area (assuming that each line is unique if it doesn't overlap with another line). Then how can the number of field lines in a particular area be a fixed quantity? This statement is contradicted by the fact that a particle will experience a magnetic force for each and every point in space. This would not be possible if at some specific points there are no magnetic field lines. The surface integral approach is clearer as some limits are taken into account and also there is no such thing as 'number of lines', but I find it very confusing when people say that the strength of the magnetic field is proportional to number of field lines/area. Why is this terminology still used? Is it because we assume that no magnetic field lines exist at places where the forces are very weak?

EDIT: Then why are there gaps between the iron filing lines? Is it because of my previous statement

because we assume that no magnetic field lines exist at places where the forces are very weak

And hence the iron filings align themselves to stronger field lines. Is this a reason why this terminology is still used?

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Best Answer

why there are gaps between the the iron filling lines?

Iron filings are ferromagnetic. They don't just show the field, they change it.

...hence the iron filings align themselves to stronger field lines.

The filings self-organize into distinct lines because their presence concentrates the field. Magnetic field lines prefer to go through a ferromagnetic body rather than through empty space. The field actually is stronger inside the iron particles than in the gaps between them.

If you drop a new filing into the gap between two of the visible "lines," it will feel attraction toward either of the surrounding lines. It will only stay put, and become the seed for a new line, if the magnetic force that it feels is too weak to overcome the static friction between the particle and the paper (or whatever) underneath.