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If magnetic field is conservative, then why not the magnetic force?

My professor thinks it is non conservative but he couldn't explain to me why?

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marked as duplicate by jinawee, Kyle Kanos, DavePhD, Qmechanic Jun 9 '14 at 14:24

This question has been asked before and already has an answer. If those answers do not fully address your question, please ask a new question.

possible duplicate of Is there any potential associated with magnetism – jinawee Jun 9 '14 at 9:13
More Phys.SE questions on conservative force and magnetism:… – Qmechanic Jun 9 '14 at 12:14

This is because of the definition of a conservative force (and links therein):

If a force acting on an object is a function of position only, it is said to be a conservative force, and it can be represented by a potential energy function which for a one-dimensional case satisfies the derivative condition

conservative force

Lets look at the magnetic field, can it be described by a scalar potential?

There is no general scalar potential for magnetic field B but it can be expressed as the curl of a vector function

${\vec{B} = \vec{\nabla} \times \vec{A}}$

So it does not fall within the definition of conservative forces.

Another view:

A force field $F$, defined everywhere in space (or within a simply-connected volume of space), is called a conservative force or conservative vector field if it meets any of these three equivalent conditions:

  1. The curl of $F$ is zero: $$\nabla \times \vec{F} = 0.$$

  2. There is zero net work ($W$) done by the force when moving a particle through a trajectory that starts and ends in the same place: $$W \equiv \oint_C \vec{F} \cdot \mathrm{d}\vec r = 0.$$

  3. The force can be written as the negative gradient of a potential, $\Phi$: $$\vec{F} = -\nabla \Phi.$$

[Proof of equivalence omitted.]

The term conservative force comes from the fact that when a conservative force exists, it conserves mechanical energy. The most familiar conservative forces are gravity, the electric force (in a time-independent magnetic field, see Faraday's law), and spring force.

Many forces (particularly those that depend on velocity) are not force fields. In these cases, the above three conditions are not mathematically equivalent. For example, the magnetic force satisfies condition 2 (since the work done by a magnetic field on a charged particle is always zero), but does not satisfy condition 3, and condition 1 is not even defined (the force is not a vector field, so one cannot evaluate its curl). Accordingly, some authors classify the magnetic force as conservative,[3] while others do not.[4] The magnetic force is an unusual case; most velocity-dependent forces, such as friction, do not satisfy any of the three conditions, and therefore are unambiguously nonconservative.

So it is not so clear, as with conservation of energy and momentum :).

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+1 I was about answering the same way... – Valter Moretti Jun 9 '14 at 9:45
+1 also; however, I can't quite see what you're referring to when you say conditions 2, 1 and 3. – gj255 Jun 9 '14 at 10:03
@gj255 it is from the wiki link before. I did not copy everything – anna v Jun 9 '14 at 11:03

This is a strange one. The magnetic field is NOT conservative in the presence of currents or time-varying electric fields.

A conservative field should have a closed line integral (or curl) of zero. Maxwell's fourth equation (Ampere's law) can be written $$ \nabla \times {\bf B} = \mu_0 {\bf J} + \mu_0 \epsilon_0 \frac{\partial {\bf E}}{\partial t}\, , $$ so you can see this will equal zero only in certain cases.

Magnetic force is also only conservative in special cases. The force due to an electromagnetic field is written $$ {\bf F} = q{\bf E} + q{\bf v} \times {\bf B}$$

For this to be conservative then $\nabla \times {\bf F} = 0$ and $$ \nabla \times {\bf F} = q\nabla \times {\bf E} + q\nabla \times ({\bf v} \times {\bf B}) .$$ But from Faraday's law we know that $$ \nabla \times {\bf E} = - \frac{\partial {\bf B}}{\partial t}\, , $$ so, $$ \nabla \times {\bf F} = - \frac{\partial {\bf B}}{\partial t} + {\bf v}(\nabla \cdot {\bf B}) - {\bf B}(\nabla \cdot {\bf v})\, .$$ From the solenoidal law $\nabla \cdot {\bf B}=0$ always, and $\nabla \cdot {\bf v} = \partial/\partial t(\nabla \cdot {\bf r}) = 0$, thus $$ \nabla \times {\bf F} = - q\frac{\partial {\bf B}}{\partial t} $$ and the force is only conservative in the case of stationary magnetic (and hence electric) fields.

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