Does the electric current have a direction?

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hmalkan
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We know that the electrical current is scalar. Also we know that a scalar hasn't got a direction but electric current has got a direction. I've confused! Please help me..
 
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Electric current does have a direction, and, as such, is a vector, and not a scalar.
 
Electic current does have a direction, the problem is the frequent appearance of the equation:

[tex]i = \frac{dq}{dt}[/tex]

which does not really tell exactly what current is; this equation only gives you the magnitude, not the direction. I prefer to define the surface current density:

[tex]\vec{j} = \rho \vec{v}[/tex]

in terms of the charge density and the velocity. Then we have:

[tex]\vec{i} = A \vec{j}[/tex]

where A is the area.
 
http://ecx.images-amazon.com/images/I/41VHYYJB0KL._SL160_.jpg

This is my book. It says electric current is a scalar at the heading of chapter 2.

 
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The current density [itex]\vec J[/itex] is a vector, but the current I through a given surface is a scalar, as can be seen from the relationship between the two:

[tex]I = \int{\vec J \cdot d \vec a}[/tex]

When you're calculating e.g. the magnetic force on a current-carrying wire, the directionality of the current is properly associated with the length of the wire rather than with the current itself:

[tex]\vec F = I \vec l \times \vec B[/tex]

for a straight wire segment and uniform [itex]\vec B[/itex], or

[tex]\vec F = I \int {d \vec l \times \vec B}[/tex]

otherwise. This assumes that [itex]\vec B[/itex] doesn't vary significantly over the cross-section of the wire. If it does, then you have to calculate the force by using the current density and integrating over the volume of the wire:

[tex]\vec F = \int {(\vec J \times \vec B) dV}[/tex]
 
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confinement said:
[tex]\vec{i} = A \vec{j}[/tex]

where A is the area.

You have to allow for the area not being perpendicular to the current. If [itex]\vec J[/itex] is uniform, then you can use

[tex]I = \vec J \cdot \vec A[/tex]

where the direction of [itex]\vec A[/itex] is perpendicular to the surface. If [itex]\vec J[/itex] is not uniform, then you have to integrate.
 
jtbell said:
The current density [itex]\vec J[/itex] is a vector, but the current I through a given surface is a scalar, as can be seen from the relationship between the two:

[tex]I = \int{\vec J \cdot d \vec a}[/tex]

When you're calculating e.g. the magnetic force on a current-carrying wire, the directionality of the current is properly associated with the length of the wire rather than with the current itself:

[tex]\vec F = I \vec l \times \vec B[/tex]

for a straight wire segment and uniform [itex]\vec B[/itex], or

[tex]\vec F = I \int {d \vec l \times \vec B}[/tex]

otherwise. This assumes that [itex]\vec B[/itex] doesn't vary significantly over the cross-section of the wire. If it does, then you have to calculate the force by using the current density and integrating over the volume of the wire:

[tex]\vec F = \int {(\vec J \times \vec B) dV}[/tex]

I don't understand what [itex]\vec B[/itex] stands for.
 
hmalkan said:
http://ecx.images-amazon.com/images/I/41VHYYJB0KL._SL160_.jpg

This is my book. It says electric current is a scalar at the heading of chapter 2.


Current is scalar.

Current (in amperes) is the amount of charge that passes through a point on a conductor every second. It is just a number. An "ampere" is a scalar quantity.

But, and this might make it confusing, but the electrons do flow in a given direction.
The electrical current does have a direction, but that information isn't contained in the unit "ampere".

Does that make sense at all? I could try to explain it better...
 
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The units only ever measure magnitude, not direction.

It doesn't even make sense to have vector units.
 
All you are very helpful. Thanks for replies.