Why is the current in a conductor equal to zero when not connected to a circuit?

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Homework Help Overview

The discussion revolves around the behavior of current in a conductor that is not connected to a circuit. Participants explore why the current is considered to be zero in such a scenario, focusing on the balance of charge flow within the conductor.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants examine the concept of current as the rate of charge transfer and question how equal flows of electrons in opposite directions result in zero current. There are inquiries about the implications of a net charge flow and the effects on charge distribution. Some suggest exploring related concepts like thermal noise and the second law of thermodynamics.

Discussion Status

The discussion is active, with participants raising questions and seeking clarification on the cancellation of charge flows. Some have provided insights into how potential differences arise and their effects on charge movement, while others express uncertainty about the implications of charge distribution changes.

Contextual Notes

Participants are navigating the complexities of charge flow in a conductor without external connections, and there are references to specific physical laws and concepts that may influence the understanding of the situation.

tellmesomething
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Homework Statement
"As there is a large number of free electrons in random directions, the number of electrons crossing an area ##\delta S## from one side very nearly equals the number crossing from the other side in any given time interval. The electric current through the area is therefore 0"
Relevant Equations
None
Can someone provide me with a justification on this? As fair as I know current through an area is the rate of transfer of charge from one side of an area to the other.
So how does current become 0 in a conductor (not connected to a circuit just a plain conductor) just cause "the number of electrons crossing an area ##\delta S## from one side very nearly equals the number crossing from the other side in any given time interval. " I dont think I understand this very well.
 
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tellmesomething said:
Can someone provide me with a justification on this? As fair as I know current through an area is the rate of transfer of charge from one side of an area to the other.
So how does current become 0 in a conductor (not connected to a circuit just a plain conductor) just cause "the number of electrons crossing an area ##\delta S## from one side very nearly equals the number crossing from the other side in any given time interval. " I dont think I understand this very well.
If there were a significant net flow of charge in one direction then what would happen to the charge distribution as a result? What would then happen to the net flow of charge?

You might also do some Googling about thermal noise.

The second law of thermodynamics has something to say as well.
 
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Relevant Equations: None
tellmesomething said:
... As fair as I know current through an area is the rate of transfer of charge from one side of an area to the other.
If
##N## electrons per second cross area ##\delta S## moving left to right,
and simultaneously
##N## electrons per second cross the same area moving right to left
then the net rate of charge flow is zero. The current is zero because the two opposite flows of charge cancel, resulting in no overall flow of charge.

Edit. @tellmesomething, just in case of possible confusion, note that the area ##\delta S## is an area inside the conductor - not an end. So ##\delta S## has metal on both sides,
 
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Steve4Physics said:
Relevant Equations: None

If
##N## electrons per second cross area ##\delta S## moving left to right,
and simultaneously
##N## electrons per second cross the same area moving right to left
then the net rate of charge flow is zero. The current is zero because the two opposite flows of charge cancel, resulting in no overall flow of charge.

Edit. @tellmesomething, just in case of possible confusion, note that the area ##\delta S## is an area inside the conductor - not an end. So ##\delta S## has metal on both sides,
Thata what I dont get, how do they cancel out, the formula is ##i=\frac{dq}{dt}##
I dont see how the signs would change. .for each of the cases you described
 
jbriggs444 said:
If there were a significant net flow of charge in one direction then what would happen to the charge distribution as a result? What would then happen to the net flow of charge?

You might also do some Googling about thermal noise.

The second law of thermodynamics has something to say as well.
I honestly don't know how the charge distribution would change? Hints?
 
tellmesomething said:
I honestly don't know how the charge distribution would change? Hints?
If you have charge moving from one side to the other, the other side will have more charge.
 
jbriggs444 said:
If you have charge moving from one side to the other, the other side will have more charge.
Right and this is when there's no cell connected to give a continuous flow of charges yes so one side would have more charge...
So are you implying this shouldnt be possible ?
 
tellmesomething said:
Right and this is when there's no cell connected to give a continuous flow of charges yes so one side would have more charge...
So are you implying this shouldnt be possible ?
What happens if you cram lots of positive charge on one side and lots of negative charge on the other?
 
jbriggs444 said:
What happens if you cram lots of positive charge on one side and lots of negative charge on the other?
A potential difference appears
 
  • #10
tellmesomething said:
Thata what I dont get, how do they cancel out, the formula is ##i=\frac{dq}{dt}##
I dont see how the signs would change. .for each of the cases you described
##\frac{dq}{dt}## is positive for charges moving (say) left to right.
##\frac{dq}{dt}## is negative for charges moving right to left.
These two flows occur simultaneously.
When you add the positve and negative values, they cancel.
 
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  • #11
Steve4Physics said:
##\frac{dq}{dt}## is positive for charges moving (say) left to right.
##\frac{dq}{dt}## is negative for charges moving right to left.
These two flows occur simultaneously.
When you add the positve and negative values, they cancel.
Oh okay. Thankyou
 
  • #12
tellmesomething said:
A potential difference appears
Does this difference assist or prevent any further movement of charge?
 
  • #13
jbriggs444 said:
Does this difference assist or prevent any further movement of charge?
Assists
 
  • #14
tellmesomething said:
Assists
So if one side of the conductor builds up a charge, it will assist in building up more charge on that side? Do we get a runaway effect?
 
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