Relationship between current and current density for a volume conductor

Cole A.
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(I'd like to preface this with the warning that the following question may be a very dumb one.)

My understanding is that current density (or flux) [itex]\vec{J} = \vec{J}(x, y, z)[/itex] is the rate of flow of charge (or the current) per unit area. (Units of [itex]\frac{\text{C/s}}{\text{cm}^2}[/itex].)

Say we know that in an irregularly shaped volume conductor (e.g. a nerve fiber, where the irregularity is due to some sort of biological obstruction), the current density [itex]\vec{J}[/itex] has the form given in Figure 1 (see attachments).

The current [itex]I[/itex] is --- I think --- given from Ohm's law: specifically, if the potential difference across the ends of the fiber and the total resistance of the fiber are known, then

[tex] \begin{equation*}<br /> I = \frac{V}{R},<br /> \end{equation*}[/tex]

which is a scalar quantity. I believe this value is constant for each point [itex](x, y, z)[/itex] in the fiber, assuming no build-up of current anywhere (by the law of conservation of charge).

Now I know that the surface integral of a flux gives a flow rate, so the surface integral of [itex]\vec{J}[/itex] should give a current. But is the current equal to [itex]I[/itex]? I mean, does

[tex] \begin{equation*}<br /> \iint_S \vec{J} \cdot \vec{n} dS = I<br /> \end{equation*}[/tex]

for every [itex]S[/itex], or only for [itex]S[/itex] = cross-sectional area of the conductor? The reason I ask is because, if I draw three example surfaces [itex]S_1, S_2, S_3[/itex] (Figure 2), the surface integral of [itex]\vec{J}[/itex] over [itex]S_1[/itex] is obviously not equal to that over [itex]S_2[/itex].

So I guess what I am asking is: is
[tex] \begin{equation*}<br /> I = \iint_{S_1} \vec{J} \cdot \vec{n} dS_1 = \iint_{S_3} \vec{J} \cdot \vec{n} dS_3 \neq \iint_{S_2} \vec{J} \cdot \vec{n} dS_2<br /> \end{equation*}[/tex]
true, where [itex]I[/itex] is current as found from Ohm's law? And if so, does this mean that any current [itex]I[/itex] through a conductor is not simply the rate of flow of charge, but a rate of flow of charge implicitly with respect to the cross-sectional area?

Thanks
 

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Cole A. said:
(I'd like to preface this with the warning that the following question may be a very dumb one.)

My understanding is that current density (or flux) [itex]\vec{J} = \vec{J}(x, y, z)[/itex] is the rate of flow of charge (or the current) per unit area. (Units of [itex]\frac{\text{C/s}}{\text{cm}^2}[/itex].)

Say we know that in an irregularly shaped volume conductor (e.g. a nerve fiber, where the irregularity is due to some sort of biological obstruction), the current density [itex]\vec{J}[/itex] has the form given in Figure 1 (see attachments).

The current [itex]I[/itex] is --- I think --- given from Ohm's law: specifically, if the potential difference across the ends of the fiber and the total resistance of the fiber are known, then

[tex] \begin{equation*}<br /> I = \frac{V}{R},<br /> \end{equation*}[/tex]

which is a scalar quantity.
Fine up to here.
Cole A. said:
I believe this value is constant for each point [itex](x, y, z)[/itex] in the fiber, assuming no build-up of current anywhere (by the law of conservation of charge).
No, this is wrong. Current I is a total amount, that is, it's the integral of J across a surface as you've written below. It doesn't make sense to talk about I at an infinitesimal point (x,y,z).
Cole A. said:
Now I know that the surface integral of a flux gives a flow rate, so the surface integral of [itex]\vec{J}[/itex] should give a current. But is the current equal to [itex]I[/itex]? I mean, does

[tex] \begin{equation*}<br /> \iint_S \vec{J} \cdot \vec{n} dS = I<br /> \end{equation*}[/tex]

for every [itex]S[/itex], or only for [itex]S[/itex] = cross-sectional area of the conductor?
In your example, it is the second option.
Cole A. said:
The reason I ask is because, if I draw three example surfaces [itex]S_1, S_2, S_3[/itex] (Figure 2), the surface integral of [itex]\vec{J}[/itex] over [itex]S_1[/itex] is obviously not equal to that over [itex]S_2[/itex].

So I guess what I am asking is: is
[tex] \begin{equation*}<br /> I = \iint_{S_1} \vec{J} \cdot \vec{n} dS_1 = \iint_{S_3} \vec{J} \cdot \vec{n} dS_3 \neq \iint_{S_2} \vec{J} \cdot \vec{n} dS_2<br /> \end{equation*}[/tex]
true, where [itex]I[/itex] is current as found from Ohm's law?
Yes.
Cole A. said:
And if so, does this mean that any current [itex]I[/itex] through a conductor is not simply the rate of flow of charge, but a rate of flow of charge implicitly with respect to the cross-sectional area?

Thanks
Yes. Usually it's obvious what that surface is (current in a wire refers to the area of the wire), but if the surface isn't obvious then you need to specify it.
 
Thank you for clearing things up.
 

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