What does B.dl indicate in Ampere's Law

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SUMMARY

The discussion clarifies that the line integral \(\oint \vec{B} \cdot \vec{dl}\) in Ampere's Law represents the circulation of the magnetic field around a closed loop. This integral is equal to \(\mu_0 \int_S \mathbf{J} \cdot dA\), where \(\mathbf{J}\) is the current density. The term does not have a specific name akin to "electric flux" in Gauss's Law, although the related expression \(\oint \mathbf{H} \cdot dl\) is referred to as "magnetomotance." Understanding these concepts is crucial for applying Maxwell's equations in electromagnetic theory.

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sawer
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I know that\oint \vec E \cdot \vec{dS} in Gauss Law indicates electric flux.
\oint \vec E \cdot \vec{dS} = \frac{Q_{enc}}{\varepsilon_0}

But what does B.dl indicate in Ampere's Law?
##\oint \vec{B} \cdot \vec{dl} ## = ??
 
Last edited:
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Such a line integral around a closed loop is the circulation of the vector field, here the magnetic field. The fundamental laws are the Maxwell equations in local form, and the Ampere-Maxwell Law reads (written in terms of the macroscopic laws in Heaviside-Lorentz units)
$$\vec{\nabla} \times \vec{H}-\frac{1}{c} \partial_t \vec{D}=\frac{1}{c} \vec{j}.$$
The integral form follows from integrating over a surface and using Stokes's integral theorem to change the curl part into a line integral along the boundary of the surface,
$$\int_{\partial F} \mathrm{d} \vec{r} \cdot \vec{H} = \frac{1}{c} \int_F \mathrm{d}^2 \vec{f} \cdot (\vec{j}+\partial_t \vec{D}).$$
For the static case, where ##\partial_t \vec{D}=0##, the right-hand side is the total electric current running through the surface under consideration.

For the non-static case, it's misleading to interpret the ##\partial_t \vec{D}## term as "source" of the magnetic field. Here you need the full (retarded) solutions of Maxwell's equations to express the electromagnetic field in terms of their sources, which are the electric charge and current densities. See, e.g.,
https://en.wikipedia.org/wiki/Jefimenko's_equations
 
Or in short
\oint \mathbf{B}\cdot \mathbf{dl}=\mu _{0}\int _{S}\boldsymbol{\mathbf{J\cdot}}\boldsymbol{dA}
The line integral of B around any loop is equal to the total current crossing any surface bounded by that loop at least for nonmagnetic materials and J >> ∂D/∂t
 
vanhees71 said:
Such a line integral around a closed loop is the circulation of the vector field, here the magnetic field.
Is there a special name for that, like in electric case, gauss law is equal to "electric flux".

##\oint \vec{B} \cdot \vec{dl} ## is not equal to magnetic flux, right?
 
gleem said:
The line integral of B around any loop is
Is there a special name for that? (Like electric flux or magnetic flux etc...)
 
I do not know of a special name for it.

However the related expression
\oint \mathbf{H\cdot dl}
is called the magnetomotance.
 
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