What does B.dl indicate in Ampere's Law

In summary, the conversation discusses the significance of the line integral in Ampere's Law, which represents the circulation of the magnetic field around a closed loop. The integral form of the law is derived from the Maxwell equations and is used to calculate the total current crossing a surface bounded by the loop. There is no special name for this specific line integral, but the related expression \oint \mathbf{H\cdot dl} is known as the magnetomotance.
  • #1
sawer
65
2
I know that[tex] \oint \vec E \cdot \vec{dS} [/tex] in Gauss Law indicates electric flux.
[tex] \oint \vec E \cdot \vec{dS} = \frac{Q_{enc}}{\varepsilon_0} [/tex]

But what does B.dl indicate in Ampere's Law?
##\oint \vec{B} \cdot \vec{dl} ## = ??
 
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  • #2
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
 
  • #3
Or in short
[tex]\oint \mathbf{B}\cdot \mathbf{dl}=\mu _{0}\int _{S}\boldsymbol{\mathbf{J\cdot}}\boldsymbol{dA}[/tex]
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
 
  • #4
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?
 
  • #5
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...)
 
  • #6
I do not know of a special name for it.

However the related expression
[tex]\oint \mathbf{H\cdot dl}[/tex]
is called the magnetomotance.
 
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Related to What does B.dl indicate in Ampere's Law

1. What is B.dl in Ampere's Law?

B.dl is a mathematical term that represents the dot product of the magnetic field vector (B) and a differential length element (dl). It is used in Ampere's Law to calculate the magnetic field around a closed loop.

2. How is B.dl different from B in Ampere's Law?

B is the magnetic field vector, which describes the strength and direction of the magnetic field. B.dl, on the other hand, is the product of B and dl, and it represents the component of the magnetic field that is perpendicular to the loop. This component is responsible for producing a magnetic flux through the loop and plays a crucial role in Ampere's Law.

3. What is the significance of B.dl in Ampere's Law?

B.dl is a key term in Ampere's Law, which states that the line integral of B.dl around a closed loop is equal to the current passing through the loop multiplied by the permeability of free space. This allows us to calculate the magnetic field at a point by knowing the current passing through a nearby loop.

4. How do you calculate B.dl in Ampere's Law?

In order to calculate B.dl, we first need to know the magnitude and direction of the magnetic field (B) and the differential length element (dl). We then take the dot product of these two vectors to get the value of B.dl. This process is repeated for each point along the loop, and the values are added together to get the total B.dl for the entire loop.

5. Can B.dl be negative in Ampere's Law?

Yes, B.dl can be negative in Ampere's Law. This can happen if the magnetic field (B) and the differential length element (dl) are in opposite directions, resulting in a negative dot product. It is important to pay attention to the direction of these vectors when calculating B.dl and to use the correct sign in the final calculation.

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