Gauss's Law for Magnetism
Source lecture(s): SC134 Lec11
Intuition
There are no magnetic monopoles—every field line that enters a volume must leave it.
Formal Definition
\[\oint \vec{B}\cdot d\vec{A} = 0\]
Mathematical Formulation
Differential form: \(\nabla\cdot\vec{B} = 0\) Consequence: \(\vec{B} = \nabla\times\vec{A}\) (vector potential exists).
Derivation
No experimental evidence for isolated magnetic charge; field lines always close.
Worked Example
Bar magnet field lines exit north, loop through space, and enter south—closed loops.
Common Mistakes
- Treating magnetic monopoles as real in introductory problems.
- Confusing with Ampere's law.
Related Concepts
Quiz
Q1. What would Gauss's law for magnetism look like if monopoles existed?
Answer
Right side would be \(\mu_0 q_m\).