Without prefix:What is the explanation for Kirchhoff's Voltage Rule?

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Kirchhoff's Voltage Rule states that the sum of voltages around a closed circuit must equal zero, reflecting the conservation of energy. The discussion highlights that as electrons flow through a circuit, they lose energy due to collisions with resistors, which results in a voltage drop. It is clarified that while transient situations may allow electrons to have some remaining energy, in steady-state conditions, the energy supplied by the battery equals the energy dissipated by resistors. The concept of zero net work in a closed loop is explained through the idea that energy is conserved, with all energy accounted for in the circuit. Overall, Kirchhoff's laws serve as approximations that hold true under steady-state conditions, despite complexities in transient scenarios.
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Hello,

I was reading the article given in this link http://www2.ignatius.edu/faculty/decarlo/kirchhoff.htm, of which pertains to Kirchhoff's Rules.

In this article, these claims are made:

"1. Voltage Rule. This is based on the conservation of energy: 'the sum of voltages around a closed conducting loop (that is, a circuit) must be zero'

In other words, since voltage and work are related, we are saying the net work done must be zero."

I understand that the battery provides the electrons with energy, that they may traverse the circuit; in addition, I understand that when the electrons (which make up the electric current) flow through the resistor collisions between the electrons and the resistor occur, which results in the electrons losing energy, corresponding to the electric potential drop. However, I don't understand why it's necessary that all of the energy is used up as the electrons flow through the circuit, isn't it possible that some (perhaps even all of them) have some remaining energy when they come to the threshold of the positive terminal?

As I attempted to answer this question, I came across this article: http://farside.ph.utexas.edu/teaching/302l/lectures/node59.html

They, too, make a claim that I am unsure of:

"This rule [voltage rule] is also easy to understand...zero net work is done in slowly moving a charge around some closed loop in an electrostatic field."

Why is zero net work done?

I'd massively appreciate it if someone could help me resolve these questions.

Thank you for your time.
 
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Hello Bashyboy! :smile:
Bashyboy said:
However, I don't understand why it's necessary that all of the energy is used up as the electrons flow through the circuit, isn't it possible that some (perhaps even all of them) have some remaining energy when they come to the threshold of the positive terminal?

"This rule [voltage rule] is also easy to understand...zero net work is done in slowly moving a charge around some closed loop in an electrostatic field."

Why is zero net work done?

energy is conserved

where do you think the energy goes? :confused:

(if, as in your example, it isn't used up, then it's still conserved, isn't it?)

since energy is conserved, that means the electric force is conservative

and voltage = electric potential = potential energy per charge

which by definition of potential energy is:

minus the work done by a conservative force, per charge​
 
Well, doesn't some of the charge go into heating up the resistor?
 
Bashyboy said:
Well, doesn't some of the charge go into heating up the resistor?

Yes, some of the energy goes into heating up the resistor.

(the charge of course is constant)

The potential drop across the resistor (V = IR) is a measure of the heat …

it tells you where the energy has gone.

The battery puts energy into the loop, the resistors take energy out of the loop, the whole thing balances.

All the energy is accounted for by KVL.
 
I still don't see how to answer my original problems. For my first question, isn't it possible that an electron is given energy by the battery, it flows through the resistor and loses some energy--but not all of it--, and goes through the entire circuit, coming to the positive terminal with some remaining energy?
 
Bashyboy said:
I still don't see how to answer my original problems. For my first question, isn't it possible that an electron is given energy by the battery, it flows through the resistor and loses some energy--but not all of it--, and goes through the entire circuit, coming to the positive terminal with some remaining energy?

Sure, that's possible. That would be a transient situation, though. When you first connect a battery to a circuit, the current through the battery isn't immediately equal to the steady-state value; instead, the current will increase from zero to the steady-state value. The steady-state value is the value for which the increase in an electron's energy caused by the battery is exactly equal to the decrease in its energy caused by the resistor. Kirkhoff's laws are approximations that ignore those sort of transient changes.
 
Bashyboy said:
… an electron is given energy by the battery … coming to the positive terminal with some remaining energy?

the battery is like the motor in a car

the resistances are like the friction in the bearings, the wind resistance, etc

when the battery, or the motor, has been running for a short time, equilibrium is reached

the speed of the car adjusts so that the energy lost to friction, wind resistance, etc, exactly equals the energy supplied by the motor

the current from the battery adjusts so that the energy lost in the resistances exactly equals the energy supplied by the battery :wink:

EDIT: stevendaryl already said it! :smile:
 
Does this somehow explain why the net work is zero?
 
The battery isn't throwing the electrons into the wire. It's not the case that the electrons move into the wire at high speed and then gradually slow down on their way to the other end. Their speed is the same everywhere in the wire assuming the diameter of the wire is equal everywhere. On their journey the electrons are constantly giving of energy to the metal atoms. Despite of that their speed doesn't change because they also are constantly receiving energy from the electric field produced by the battery. The electrons move very very slowly, so their kinetic energy is virtually zero. They can't have any energy left when they reach the end of the wire because they never really had any energy to begin with. When you use a rope to pull a heavy object you have to put a lot of energy into overcome the friction but the rope never really had much energy since it's very light and moves slowly. So when you stop pulling will the rope have any energy left in it?

Bashyboy said:
"This rule [voltage rule] is also easy to understand...zero net work is done in slowly moving a charge around some closed loop in an electrostatic field."

Why is zero net work done?

This rule does not apply to an electric field that's induced by a changing magnetic field e.g. a transformer. In that case charge that moves around the transformer core in a closed loop will have work done on it. Such a field is called "non conservative". There is a great video about that topic here


Most electric fields however are conservative fields. That means that in a closed loop no net work is done on a charge. That is because of conservation of energy. Imagine you had two objects that are statically charged and then you take a third charged object and let it move in a circle between the other two. If it was receiving energy on it's path it could continue to circle forever and you would get energy from nothing.
 
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  • #10
Bashyboy said:
"This rule [voltage rule] is also easy to understand...zero net work is done in slowly moving a charge around some closed loop in an electrostatic field."

Why is zero net work done?

I'd massively appreciate it if someone could help me resolve these questions.

Thank you for your time.
I honestly think that it is confusing to explain the voltage rule in circuits with the work by charge in electrostatic field. At least one shouldn't think they are literaly the same. Rather, the charge moving in closed loop in the electric field is just analogy to charge moving across the closed circuit.
But I might be wrong.
 
  • #11
stevendaryl said:
Sure, that's possible. That would be a transient situation, though. When you first connect a battery to a circuit, the current through the battery isn't immediately equal to the steady-state value; instead, the current will increase from zero to the steady-state value. The steady-state value is the value for which the increase in an electron's energy caused by the battery is exactly equal to the decrease in its energy caused by the resistor. Kirkhoff's laws are approximations that ignore those sort of transient changes.

Using the idea that electrons are flowing around a circuit (although there is a mean drift speed, of course) in conjunction with the idea of a "transient situation" can hardly make sense. During any 'switch on' settling time (as little as a few ns duration for some circuits) an electron would hardly have traveled by any significant distance (10-12m, typically). This is just another example of how discussing electric currents in terms of electrons can be nonsensical. Just stick to Current and 'charges' and worry about electron movement when it is relevant - like inside solid state and thermionic devices (black boxes when doing circuit analysis).
 
  • #12
Bashyboy said:
Does this somehow explain why the net work is zero?

Yes it does. If all the energy supplied by the battery were not dissipated or transferred within the circuit, where would it go or where would any extra energy come from?
 
  • #13
xAxis said:
I honestly think that it is confusing to explain the voltage rule in circuits with the work by charge in electrostatic field. At least one shouldn't think they are literaly the same. Rather, the charge moving in closed loop in the electric field is just analogy to charge moving across the closed circuit.
But I might be wrong.

Absolutely. A 9V battery, 0.02m long would have a field of 9/0.02V/m across its terminals. Another, physically bigger, battery - say 0.1m long, would have 1/5 of the electric field across its terminals. How could anyone invent a system for circuit analysis that worked on the basis that different batteries of the same voltage would produce different resuts. (Not to mention the lengths of the connecting wires in a DC circuit)
We use Volts, Potential Difference and Energy transferred etc etc because it works and Volts per Metre wouldn't work.
Volts per Metre becomes relevant in many instances, such as electron tubes and particle accelerators but it's 'horses for courses' in Science.
 
  • #14
sophiecentaur said:
Using the idea that electrons are flowing around a circuit (although there is a mean drift speed, of course) in conjunction with the idea of a "transient situation" can hardly make sense.

I don't think you're really addressing his question. He's asking about the claim that conservation of energy implies that the changes in voltages around a circuit add up to zero. It's true that for the domain of applicability of Kirkhoff's laws that the voltages add up to zero, but it doesn't follow from conservation of energy.
 
  • #15
stevendaryl said:
I don't think you're really addressing his question. He's asking about the claim that conservation of energy implies that the changes in voltages around a circuit add up to zero. It's true that for the domain of applicability of Kirkhoff's laws that the voltages add up to zero, but it doesn't follow from conservation of energy.

But his question involves an assumption that there is a reasonable answer in terms of electrons buzzing through the wires. I don't think there is one in those terms.
 
  • #16
sophiecentaur said:
Yes it does.

No, it doesn't.

If all the energy supplied by the battery were not dissipated or transferred within the circuit, where would it go or where would any extra energy come from?

Conservation of energy just says that the energy drained from the battery must equal the energy in the circuit minus the energy dissipated away by the resistors. To get that the energy drained from the battery is equal to the energy dissipated away, you have to assume that the energy in the circuit doesn't keep getting greater.

Mathematically, energy is being supplied by the battery at the rate

I V_{battery}

Energy is being dissipated by the resistor at the rate

I^2 R

To get these two equal, you need the assumption that the total energy in the circuit doesn't change with time. That will not absolutely true for all times, but it will be true to a very good approximation soon after the battery is connected.
 
  • #17
Bashyboy said:
I don't understand why it's necessary that all of the energy is used up as the electrons flow through the circuit, isn't it possible that some (perhaps even all of them) have some remaining energy when they come to the threshold of the positive terminal?[/B]

I just read this part of your OP. If there were any resistance in the contact with this terminal then the voltage at this point would not be zero. (And, of course, all real batteries do have some internal resistance so, once you start to drain current from them, some energy is, in fact, dissipated internally, so there is some energy 'left' after the charge has 'passed around' a real circuit.
I wonder if part of your problem with this is that you are thinking in terms of the 'electrons' carrying the energy round the circuit in the form of Kinetic Energy? This is a common misconception which can be resolved once one considers their 1mm/s mean drift speed and the total mass of moving electrons in a wire (1/120,000 of the mass of a copper wire they are moving through).
 
  • #18
SO the energy in the circuit turns up in the form of magnetic or electric fields and they need to be included in the Kirchoff analysis. But K2 only applies where there is a conservative field. The OP was referring to the simple model of a battery and some resistors. Adding extra factors can't help in explaining the basic concept, surely.
 
  • #19
sophiecentaur said:
But his question involves an assumption that there is a reasonable answer in terms of electrons buzzing through the wires. I don't think there is one in those terms.

His question was why does conservation of energy imply that the sum of voltage changes around a circuit must add up to zero? He was trying to understand this by using a picture of electrons moving through the circuit, but his question is perfectly valid, however you try to understand it. How does one prove, from conservation of energy alone, that the sum of voltage changes around a loop add up to zero? You can't prove it from conservation of energy alone. If you let U_{battery} be the internal energy of the battery, and U_{circuit} be the internal energy of the circuit, then conservation of energy tells us that:

\dfrac{d}{dt} U_{total} = - I^2 R

where U_{total} = U_{battery} + U_{circuit}.

The additional assumption that's needed is something along the lines that
U_{circuit} = 0 for a perfect conductor. There is no energy associated with having current flowing through a wire. It's not exactly obvious that that's true, and I don't think it is precisely true, but it's approximately true, because as you say, the charges in a conductor don't move very far at all, so there's really no way to build up kinetic or potential energy inside a conductor.
 
  • #20
sophiecentaur said:
I just read this part of your OP. If there were any resistance in the contact with this terminal then the voltage at this point would not be zero. (And, of course, all real batteries do have some internal resistance so, once you start to drain current from them, some energy is, in fact, dissipated internally, so there is some energy 'left' after the charge has 'passed around' a real circuit.
I wonder if part of your problem with this is that you are thinking in terms of the 'electrons' carrying the energy round the circuit in the form of Kinetic Energy? This is a common misconception which can be resolved once one considers their 1mm/s mean drift speed and the total mass of moving electrons in a wire (1/120,000 of the mass of a copper wire they are moving through).

It's not a "misconception", it's a question. He's essentially asking whether there can be energy in the form of kinetic energy of charges in a circuit that increases with time as the battery is connected. The answer is that the additional kinetic energy due to drift velocity is completely negligible in ordinary circuits, and this energy is therefore ignored in Kirchoff's laws.
 
  • #21
I wouldn't argue with that at all. But trying to start an explanation (not yours) from a flawed basis (i.e. that the motion of the electrons is relevant) is not going to be helpful for anyone. Quasi mechanical pictures of circuit behaviour can only get in the way of a proper understanding and I think it's always worth while trying to steer people away from them.
It's this nagging problem of 'some energy being left over' which is so attractive - particularly if you have a picture of stuff flowing round a circuit like water (which, of course, always has some energy left after going through a water wheel etc - because it has to get out of the way to make room for the next lot coming out).
 
  • #22
stevendaryl said:
It's not a "misconception", it's a question. He's essentially asking whether there can be energy in the form of kinetic energy of charges in a circuit that increases with time as the battery is connected. The answer is that the additional kinetic energy due to drift velocity is completely negligible in ordinary circuits, and this energy is therefore ignored in Kirchoff's laws.

I think the OP can answer for himself, whether it is a question or a question based on a misconception. But, as we seem to be agreeing about the actual facts, what's the problem? :smile:
 
  • #23
sophiecentaur said:
I wouldn't argue with that at all. But trying to start an explanation (not yours) from a flawed basis (i.e. that the motion of the electrons is relevant) is not going to be helpful for anyone.

Sure, but to me, the appropriate response was something like: applying a voltage across a wire makes a negligible change in the kinetic energy of the charges in the wire, for such and reason.

In a certain sense, though, the reason drift velocity is so low is because the conductor isn't perfect, it has resistance.
 
  • #24
@stevendary
OK, I'll use you as my sub-editor in future. :wink:
 
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  • #25
stevendaryl said:
Sure, but to me, the appropriate response was something like: applying a voltage across a wire makes a negligible change in the kinetic energy of the charges in the wire, for such and reason.

In a certain sense, though, the reason drift velocity is so low is because the conductor isn't perfect, it has resistance.

The drift velocity is a consequence of the charge density and the total rate of charge transfer.
See this link (or any textbook)
The resistance is not relevant.
 
  • #26
I haven't read all of the posts, but stevendaryl was correct: my question was, "why does conservation of energy imply that the sum of voltage changes around a circuit must add up to zero?" In my query, I proposed the situation with the electron, hoping it was correct and that someone might be able to answer my questions in terms of that situation. But, if that wasn't possible, I was fine with that.
 
  • #27
sophiecentaur said:
The drift velocity is a consequence of the charge density and the total rate of charge transfer.
See this link (or any textbook)
The resistance is not relevant.

That doesn't make any sense to me. By "total rate of charge transfer", do you mean "current"? If so, then current is inversely proportional to the resistance.

In this article, the claim is made that drift velocity is proportional to the mean-free path d between collisions.

http://hyperphysics.phy-astr.gsu.edu/hbase/electric/ohmmic.html

The conductivity (the inverse of the resistance) is similarly proportional to the mean free path, and so we have:

v_d \propto \dfrac{1}{R}

So what you said is, I believe, completely wrong.
 
  • #28
sophiecentaur said:
I think the OP can answer for himself, whether it is a question or a question based on a misconception. But, as we seem to be agreeing about the actual facts, what's the problem? :smile:

The problem I have is that after reading your post, one feels more confused than when he started, and yet feels embarrassed to ask clarifying questions, for fear of being ridiculed. That's just the impression I get.
 
  • #29
Bashyboy said:
I haven't read all of the posts, but stevendaryl was correct: my question was, "why does conservation of energy imply that the sum of voltage changes around a circuit must add up to zero?" In my query, I proposed the situation with the electron, hoping it was correct and that someone might be able to answer my questions in terms of that situation. But, if that wasn't possible, I was fine with that.

stevendaryl, have you seen my message that I posted, just moments before you posted yours?
 
  • #30
Bashyboy said:
stevendaryl, have you seen my message that I posted, just moments before you posted yours?

I think that the answer is that there is negligible energy in the circuit in the form of kinetic energy of charges, because the drift velocity is so small, typically.

Conservation of energy would tell us that:

\sum_i P_i = \dfrac{dU}{dt}

where P_i is the power generated or consumed by component i, and U is the energy in the circuit in the form of kinetic energy of charges. So since the kinetic energy of charges is negligibly changed by applying a voltage, we can approximate:

\dfrac{dU}{dt} = 0

So we get:

\sum_i P_i = 0

The power P_i generated or consumed by component i is just equal to I_i V_i, where I_i is the current through component i, and V_i is the voltage change from one end of the component to the other. So we have:

\sum_i I_i V_i = 0

For a circuit without junctions that split the current, the current is the same for all components, so we would have:

\sum_i I_i V_i = I \sum_i V_i = 0
\Rightarrow \sum_i I V_i = 0

To extend the argument to the case of circuits with junctions is more work, but I assume something similar applies.
 
  • #31
Well current is indeed inversely proportional to resistance , voltage is directly proportional to current and
I think sophiecentaur is not necessarily wrong in this case as the amount of current is associated with the drift velocity , so as the current gets higher the velocity also increases and the heat dissipated by the conductor will also increase as heat is a property which arises from the kinetic energy of particles in a piece of matter as we know.
So basically it all ties up.

Now we had a debate with sophiecentaur on some earlier posts whether using electrons as describing electricity and current is useful for the inexperienced or layman and I do partly agree to him that for starters we shouldn't use quantum mechanical objects one of which is the electron.
Although this is a thing that must be left in the hands of the OP to decide, if he or she is comfortable and capable of understanding answers given by electrons not current and voltage then we should provide the answers in a way that the OP wants or has asked us to do so.If he or she hasn't said in how complicated terms the answers should be then we should ask which is actually what i have seen done here by many professional responders.
 
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  • #32
stevendaryl said:
The problem I have is that after reading your post, one feels more confused than when he started, and yet feels embarrassed to ask clarifying questions, for fear of being ridiculed. That's just the impression I get.

I apologize for the rudeness of that post.
 
  • #33
i don't think the post was rude I just think a little misunderstanding arose in this discussion
 
  • #34
Crazymechanic said:
Well current is indeed inversely proportional to resistance , voltage is directly proportional to current and
I think sophiecentaur is not necessarily wrong in this case as the amount of current is associated with the drift velocity , so as the current gets higher the velocity also increases and the heat dissipated by the conductor will also increase as heat is a property which arises from the kinetic energy of particles in a piece of matter as we know.
So basically it all ties up.

Now we had a debate with sophiecentaur on some earlier posts whether using electrons as describing electricity and current is useful for the inexperienced or layman and I do partly agree to him that for starters we shouldn't use quantum mechanical objects one of which is the electron.
Although this is a thing that must be left in the hands of the OP to decide, if he or she is comfortable and capable of understanding answers given by electrons not current and voltage then we should provide the answers in a way that the OP wants or has asked us to do so.If he or she hasn't said in how complicated terms the answers should be then we should ask which is actually what i have seen done here by many professional responders.

That's nice to know :wink:

I had the luxury, in my early education, of not being 'allowed' to try to get to grips with electricity by using electrons. It has been a real help all my life. Once I got on a degree course, it was obvious that they are not the way into the subject and I never experienced any conflict.
A few decades ago, someone decided that everything Scientific could be explained in terms of particles, when talking to young would-be Scientists. It got into School curricula and has been responsible for such a lot of confusion ever since. This is because the massive step between the observed phenomenon and the QM description (or 'quasi' QM description, rather) is too much to cope with in one go. When you get down to it, I think I'd actually prefer the water analogy for electricity than the totally half-arsed analogy that people get sold, involving electrons. These 'electrons' that are used in the model are nothing like the real thing. They have significant mass (like peas) and their motion (at almost light speed) is represented by animated dotted lines around a circuit in a movie. They just beg to be assigned momentum, Kinetic Energy and significant masses and they 'bump into' atoms on the way round a circuit, to represent resistance. Madness.
Anyone who claims to have a good explanation about any electrical phenomenon, based on that model, should just try to find it echoed in any reputable Science textbook - and they consider why they can't find it. Time to re-consider that particular approach, I think.
 
  • #35
From this discussion, I am getting the impression that the battery, in some way, provides the an electron (or current) with enough energy to make it around the circuit. It's as if the battery knows that there are resistors, and compensates for this by providing more energy than the current (or electron) would need if there were no resistors. Is this correct?
 
  • #36
Bashyboy said:
From this discussion, I am getting the impression that the battery, in some way, provides the an electron (or current) with enough energy to make it around the circuit. It's as if the battery knows that there are resistors, and compensates for this by providing more energy than the current (or electron) would need if there were no resistors. Is this correct?

All the battery needs to "know" is how much current is needed to maintain its voltage across its terminals. It hasn't a brain with which to 'know anything' but charges are produced (internally) at its terminals until the current it releases is limited by the PD that exists (externally) at its terminals. How long it takes for that voltage to appear will be determined by the step response of the circuit. This could be a few ns or ten days. This is where the idea of trying to explain the process in 'mechanical' terms becomes pointless.
Kirchoff does not claim to apply at switch-on so why try to reconcile what it says with the switch on situation or to prove him 'wrong', in some way?

There are always resistors in a circuit that Kirchoff II describes. Read it.
 
  • #37
I think the battery nor the circuit doesn't know anything , the electricity just flows from the highest potential to the lowest , because she always does that.Just like a river runs downhill not uphill.

Also the battery doesn't try to compensate for anything she just does her chemical reactions and current flows until the reactions are over and so is current.
 
  • #38
There are many models one can use to analyze a situation. e.g. kirchhoffs rules, the charge model, electron model, etc. In engineering you should always use the model that can solve a given problem with the least effort. Otherwise things just become more complicated than necessary.
Sure the charge carrier/electron model is the more fundamental one. i.e. You can derive kirchhoffs laws from the charge carrier model but not the other way around, but it's not a good choice for designing electric circuits.

However there is no reason not to discuss what's happening on the level of electrons if you are interested in that.
To understand why electrons behave the way they do you need to look at the electric fields. Let's say you have a battery and a wire with a high resistance connecting it's two terminals. The wire's diameter is equal everywhere.
Now the current will be equal everywhere in the wire and the electrons will move at an equal speed everywhere. Electrons in a wire do not behave like water molecules in a pipe. They do not simply bump into each other and thereby pushing each other along. They are always moved by an electric field. The current density in metal is ALWAYS equal to the electric field strength inside the metal times the conductivity.
That means the electric field inside the wire must be equal everywhere.

But that seems strange since the electric field of a battery should look like the magnetic field of a magnet. i.e. it should be stronger close to the battery and weaker further away. So how can it be equal over the entire length of the wire? There is only one possible solution. There is "static charge" on the surface of the wire that is distributed such that the superposition of the field of the battery and the field of the charges produce a field that is equal everywhere in the wire.
If you have a network of resistors those "static charges" will distribute themselves such that an equilibrium is reached i.e. all the currents are such that the "static charges" do not change anymore. That equilibrium is reached when kirchhoffs laws are fulfilled.

Bashyboy said:
It's as if the battery knows that there are resistors, and compensates for this by providing more energy than the current (or electron) would need if there were no resistors. Is this correct?

The battery always provides the same amount of energy independantly of the resistance. Some of that energy may be released in the internal resistance of the battery though.
If we replace the wire in my example with one made from a metal with higher resistivity, the electrons will move through it at a slower speed but will experience more "friction". But in total the energy they receive from the battery and the energy they release into the wire will stay the same.
 
  • #39
DrZoidberg said:
But that seems strange since the electric field of a battery should look like the magnetic field of a magnet. i.e. it should be stronger close to the battery and weaker further away. So how can it be equal over the entire length of the wire? There is only one possible solution. There is "static charge" on the surface of the wire that is distributed such that the superposition of the field of the battery and the field of the charges produce a field that is equal everywhere in the wire.
If you have a network of resistors those "static charges" will distribute themselves such that an equilibrium is reached i.e. all the currents are such that the "static charges" do not change anymore. That equilibrium is reached when kirchhoffs laws are fulfilled.

.

That's a good way to look at it.
It's like a string of capacitors, connected between the wires, in parallel. The Electric field between the wires (in V/m) will depend upon the spacing (can vary wildly, over the circuit) and will be far greater than the fields within the wire. It's only when you get to the Resistor that the 'series' field becomes significant.
 
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