# Ampere's Law: Any surface? But what about these? There must be some requirements right?

I was a bit confused by the fact that we can use a surface of any boundary for Ampere's law; especially when it comes to capacitance.

Consider the standard model of the capacitor used to derive the need for displacement current. Then Ampere's law, if we use the disk bounded by a circle with radius less than the plates, should have magnitude $$B = \frac{\mu_0}{2\pi} \frac{r}{R^2} i_C$$ according to my textbook. I completely understand the derivation there. But since Ampere's law could be the boundary of any surface, why couldn't we just make it into a bulging one with the same circular boundary, but with a surface which passes through the plates passes through plates and encompasses the current $$i_C$$ (surface 1)?

It feels wrong because the surface is intersecting a plate, but I read somewhere that any surface works; So, why not this one? Then only $$i_C$$ passes through the current, and $$B$$ in that reduced radius wouldn't need that factor.

What's stopping us from making a surface with that boundary that just bulges out wide then contracts (surface 2)? For more context, I'll describe what I'm thinking with some pictures below. I know there must be some misunderstanding on my part on the whole idea of bounding a surface, or there are some requirements on the surface that I'm missing, but someone please explain.

• Made some edits for easier reading Dec 19, 2020 at 12:35
• Surface-2 can't be easily distinguished from surface-1. A suggestion is to label surfaces as $S_1$ and $S_2$ Dec 19, 2020 at 12:36
• Hm. I uncapitalized the "according" since it's part of the previous sentence. I appreciate the other stylistic edits a lot, though. As for the surfaces, I'll see what I can do. Thank you! Dec 19, 2020 at 12:36
• I think the problem is not even about the ampere's law but rather the nature of current through the plate of capacitor and finding a notion of the field in there Dec 19, 2020 at 12:42
• Hm. Perhaps. I'm a bit tired right now, so I'll wait a little to see how people respond. Dec 19, 2020 at 12:56

Ampere's law does work for those surfaces too. What you have forgotten about is (i) the non-zero conduction current in the plates for surface 1; (ii) the non-zero displacement current term over surface 2. Both of these terms contribute negatively to the RHS of Ampere's law and hence match the $$r^2/R^2$$ reduction factor in the derived B-field between the plates at a distance $$r$$ from the centre line.

Ampere's law is not that the closed line integral of the B-field equals the enclosed current; it is that it is equal to the sum of the enclosed current and the enclosed displacement current terms - that is the whole point of the capacitor example. i.e. $$\oint \vec{B}\cdot d\vec{l} = \mu_0 \left(I_c + I_d\right)\ .$$

Let's simplify surface 1 to be a cylinder extending from your loop of radius $$r$$ so that it ends outside the plates. (See below for a sketch). For an ideal capacitor the electric field lines and the rate of change of electric field are parallel and run between the plates, so for surface 1 as shown above, the E-field would always be tangential to that part of the cylinder's curved surface between the plates and since there is also no electric field outside the plates there would be no displacement current term at all. However, there is obviously still the $$I_c$$ conduction current through the flat face of the cylinder contributing to the RHS of Ampere's law case, so how can we square that with the smaller value of the toroidal B-field for the Amperian loop between the plates?

Well, what you cannot assume is that there is zero conduction current in the plates themselves. For example if the capacitor plates are circular with radius $$R$$ and your circular path is of radius $$r$$, then a fraction $$(R^2 -r^2)/R^2$$ of the charge on the plates lies outside the cylindrical surface I defined above. But if the charge on the plates is changing with time there must be a net current flowing from the outer part of the plates to the inner part and then into the wire (shown as a blue current density in the picture). This will be a negative term on the RHS of Ampere's law because it flows into the cylindrical surface, and will be of size $$I(r^2 -R^2)/R^2$$. The sum of the conduction current terms is therefore smaller and indeed will match the reduced B-field between the plates at radius $$r$$ compared with the field you would expect for a similar loop outside the plates.

For surface 2 the solution is different. The surface does not cut through the plates at all so there is no additional conduction current term. However here there is a negative displacement current contribution due to the integral of the rate of change of E-field over that part of surface 2 which is between the plates. It is a negative contribution because the E-field lines are going into surface 2 between the plates. Again, a careful calculation would show that this negative displacement current plus the conduction current that exits surface 2 outside the plates is exactly what is required to balance the smaller LHS of Ampere's law for the small loop of radius $$r$$ between the plates.

• Ah, but here I was also confused. If there is a displacement current added, then why is the value derived from a disk, what I have above, less than that which comes from considering $i_C$ which passes through the surfaces, mainly $B = \frac{\mu_0}{2\pi} \frac{1}{r} i_C$ (as if the wire weren't even there)? That's what I was confused. There must be some negative? But how does that work? Dec 19, 2020 at 12:52
• @mijucik As I say in my answer, for surface 2, the displacement current term is negative because the E-field lines are going into the surface you have defined. Dec 19, 2020 at 12:57
• Oh! Sorry I missed that part. That makes so much more sense! Thank you :) Dec 19, 2020 at 12:57
• Are you saying there is a displacement current per area density between capacitor plates in the last paragraph? Also could you explain this part "Surface 1 is more interesting, especially if you just make it a cylinder poking out from the plates, such that the E-field is always tangential to the surface between the plates, since then there is no displacement current term at all. " I'm having a hard time visualizing the cylinder that you are referring too, I think a picture will help. Dec 19, 2020 at 13:05
• Just to clarify, the (and forgive me if I'm using this term wrong) induced current in the internal plates is in the opposite direction of $i_C$ right? So I can think of a small current of the value you derived as a mini one within the plates in the opposite direction? Dec 19, 2020 at 13:16

You have understood something very important. It seems like a paradox that we can use the surface through the capacitor through which no current passes. This is the crucial observation that lead to Maxwell to his equations. The point is that the validity of Ampere's law requires an extra term $${\bf J}\to {\bf J}+ \frac{\partial {\bf D}}{\partial t}$$ where $${\partial {\bf D}}/{\partial t}$$ is Maxwell's displacement current. Although there is no current $${\bf J}$$ between the plates, there is a displacement current, and once you include that you get the same $$\int {\bf H}\cdot d{\bf r}$$ for every surface.

Without the displacement current there would be no electromagnetic waves. So Maxwell's (and now your) worry about this point is the birthplace of all radio technology.

• Ah! Thank you for this extra insight into displacement currents. I really appreciate it :) I was more confused about the seeming contradiction that occurs when we assume displacement current to exist. I know I didn't ask my question clear enough, but see my above comments to Rob to kinda understand it better. Thank you again though, I really appreciate it!! Dec 19, 2020 at 12:55

This actually applies in any dimension, not just three. It goes like this.

Circulation is a kind of idea, that if you put two loops side by side, each carrying the same current, the current down the common edges cancel out, and the two polygons merge into one. Thus a figure can be built up, such that all of the polygons on the surface have currents that cancel out.

Each bit of surface, has an out-vector, which is proportional to the area. A vector normal. This vector, in a closed figure, is the 'gradient of density', or $$\nabla D$$. The interesting thing here is that for a closed surface, $$dV = \vec r \cdot d\vec S$$ , which is the usual way of measuring volume (ie sum over the volume).

Since this is a moment (that is, the sum of vector elements over coordinates), and volume does not have a residual moment, then $$\sum d\vec S = 0$$.

If we now divide the surface by a boundary, such as a loop, then there is a 'current' in the loop, and the two halves have an area-vector of $$+A$$ and $$-A$$, retaining the same value. We can then replace $$+A$$ by any other surface that is bounded by the loop, and expect that it has a definite volume, and thus has the same vector area.

It works in all dimensions. For example, given two points A and B, the vector sum of the perpendiculars to dS, segments of the line, must be constant (and equal to the length). In four dimensions, a polyhedron made of clockwise faces, points 'down', and when two clockwise faces are placed together, they cancel out.

• Wow. I've never seen it put like that. Thanks for the insight :0 Dec 19, 2020 at 12:58
• Nor had I until i discovered the therom. Dec 19, 2020 at 13:02
• Do you remember what source you learnt it from? Just wondering ~ Dec 19, 2020 at 13:02
• When I say i discovered it, it was brand new from my own hand. Dec 19, 2020 at 13:04
• fixed the equations, the D was sperious. $\nabla D = \vec S$ Dec 19, 2020 at 14:09