Potential difference across parallel circuits

In summary, the potential difference across individual components in a parallel circuit is the same due to the definition of potential difference and the fact that all wires in a circuit are assumed to be ideal. This means that if two components share the same terminals, the potential difference across them will be the same. This can be seen in the example of two resistors of different resistance connected in parallel, where the resistor with less resistance will have more current and therefore dissipate more power. The explanation for this phenomenon lies in the ratio of work done by the charges to the amount of charges, which is always the same in parallel branches. However, it should also be noted that real wires have finite resistance, which can affect the voltage measured across parallel components.
  • #1
truewt
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I am currently having some difficulty in recalling/understanding the potential difference across parallel circuits. Why is the potential difference across individual components of the parallel circuit the same?

Let's for example say 2 resistors of different resistance are connected in parallel. As p.d. is defined as the amount of energy dissipated by the charges as they pass through the resistor (am I wrong in the definition?), why is it so that for different resistances, the energy dissipated by the charges are the same?
 
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  • #2
truewt said:
I am currently having some difficulty in recalling/understanding the potential difference across parallel circuits. Why is the potential difference across individual components of the parallel circuit the same?

i am not sure what you mean by "individual components" but remember in a circuit diagram, all wires are assumed to be ideal and so if you elements share the same set of terminals (ie. parallel to each other) than the potential difference across them will be the same (by definition)


Let's for example say 2 resistors of different resistance are connected in parallel. As p.d. is defined as the amount of energy dissipated by the charges as they pass through the resistor (am I wrong in the definition?), why is it so that for different resistances, the energy dissipated by the charges are the same?

well the resistor with less resistance will let more CURRENT through and the same potential difference means that more power will be dissipated on this device compare to the other one.
 
  • #3
So what is the explanation for saying the potential difference is equal?
 
  • #4
An alternate picture of viewing parallel connected components in this case (2 resistors) is to picture each of the resistors connect [individually] directly across the terminals of the voltage source. When you think of it this way, its roughly like a series circuit; hence the voltage drop across a single resistor is equal to that of the voltage source. Taking this thinking further, its obvious that the p.d across both resistors would be equal, however the current would not be [given unequal resistances].
 
  • #5
@ranger: That could be a way, but is there a better explanation for the potential differences being equal?

I'm trying to find the best argument for this concept. I can hardly remember what my teacher explained (or did he?) a few years back.

Basically what I'm saying is why are the charges in the circuit so smart as to be able to dissipate the same amount of energy?

Let's take another example. 3 resistors are in a circuit. 2 are in parallel, and the last resistor is in series with the 2 parallel resistors. Why are the charges (which split up into separate branches in the parallel component) able to 'use up' the same amount of energy (ie the pd drop) and then join back into the main branch at the same potential?
 
  • #6
Basically what I'm saying is why are the charges in the circuit so smart as to be able to dissipate the same amount of energy?

V = W/q; where W is work (joules) and q is unit of charge [moved]. As you know the amount of charge will vary depending on the resistance in the circuit. Now if we have a 10V source, so that's 10 joules of work per coulomb of charge. If we have 3 coulomb of charge flowing in one branch:
V = 30J/3q = 10J/C = 10V
[C = coulomb which is the unit of charge; J/C = V]
If in that very same circuit, on a different branch we have 7 units of charge. This will give an electric potential of:
V = W/q = 70J/7q = 10J/C = 10V.

Makes sense?
 
  • #7
Hmm, I have wondered about this too and I thought of an explanation that might work. Think about this, the electrons in the main branch tries to move forward and when it comes to the split point, the electrons in the wire will exert an equal force to the electrons in each parallel circuit. So the potential difference for each circuit is the same.
 
  • #8
truewt said:
Let's take another example. 3 resistors are in a circuit. 2 are in parallel, and the last resistor is in series with the 2 parallel resistors. Why are the charges (which split up into separate branches in the parallel component) able to 'use up' the same amount of energy (ie the pd drop) and then join back into the main branch at the same potential?

Why is it so that the ratio between the work done by the charges and the amount of charges (ie the pd) always the same in the branches of the parallel component?
 
  • #9
truewt said:
Why is it so that the ratio between the work done by the charges and the amount of charges (ie the pd) always the same in the branches of the parallel component?

First of all, remember that real wires have some small but finite resistance. So depending on how you connect up the parallel components, they may see slightly different voltages across them depending on how much voltage drop there is in the interconnections. This is what you should use to answer your original question -- ask yourself what the resistance of the interconnections is, compared to the resistance of the components that are connected in parallel. If you use 30AWG (tiny) wire to wire up a bunch of 1 Ohm power resistors "in parallel", with 100cm space between each resistor, and the first resistor adjacent to the power supply, then you will not measure the full power supply voltage 9m away at the end resistor...

And in your quoted question here, I think you are asking about the ratio of the power in a branch to the current in the branch? When you say "charges", I think you mean the flow of the charges with respect to time, right? If so, P=VI should answer the question, right. P/I=VI/I=V, which is the same across all branches...
 
  • #10
berkeman said:
First of all, remember that real wires have some small but finite resistance. So depending on how you connect up the parallel components, they may see slightly different voltages across them depending on how much voltage drop there is in the interconnections. This is what you should use to answer your original question -- ask yourself what the resistance of the interconnections is, compared to the resistance of the components that are connected in parallel. If you use 30AWG (tiny) wire to wire up a bunch of 1 Ohm power resistors "in parallel", with 100cm space between each resistor, and the first resistor adjacent to the power supply, then you will not measure the full power supply voltage 9m away at the end resistor...

And in your quoted question here, I think you are asking about the ratio of the power in a branch to the current in the branch? When you say "charges", I think you mean the flow of the charges with respect to time, right? If so, P=VI should answer the question, right. P/I=VI/I=V, which is the same across all branches...

Hmmm, to the first part of your answer, it is right. But usually we assume ideal conditions and the wires have no resistance..

As for the second part of your reply, the point I'm asking is that why is the voltage the same? why is the work done per unit charge across each resistors in the parallel circuits the same?
 
  • #11
truewt said:
As for the second part of your reply, the point I'm asking is that why is the voltage the same? why is the work done per unit charge across each resistors in the parallel circuits the same?

Why is the voltage the same? We already answered that. Because the interconnection resistance is negligible compared to the parallel component resistances. To get a voltage drop, you need current flowing through a resistance. V=IR, so if R is negligible, the V is too.

I also already answerd the second question. P/I=VI/I=V, which is the same for all branches.

Let's try the second one a different way to see if it helps. Let's say that you have a single resistor of value R across the power supply, so obviously I=V/R, and P=VI=V^2/R. Now split that resistor into two parallel resistors of value 2R each, so the total I=V/R still, but now I/2 flows through 2R in each of the two parallel branches. Do you see where I'm going with this? What do you do next in this exercise to show the property that you are asking about? What is the current in each of the 2 parallel legs? What is the power in each of the two split legs compared to the original power in the single R before the split? Does that make it more intuitive?
 
  • #12
truewt said:
I am currently having some difficulty in recalling/understanding the potential difference across parallel circuits. Why is the potential difference across individual components of the parallel circuit the same?

Let's for example say 2 resistors of different resistance are connected in parallel. As p.d. is defined as the amount of energy dissipated by the charges as they pass through the resistor (am I wrong in the definition?), why is it so that for different resistances, the energy dissipated by the charges are the same?

Imagine a water pump hooked up to two pipes, in a configuration as like the one below with my beautiful ASCII art.

---W------________======B=======
|--------|___A___//_______________\\
|--------|======__________________=====D===
|--------|_______\\_______________//
----------________======C=======


If the water pump is W, and B and C are equal pipes. What would be the water pressure through A? What about the pressure at B and C. How would the flow of water change through B and C? What would the flow through A be compared to D?
 
  • #13
berkeman said:
Why is the voltage the same? We already answered that. Because the interconnection resistance is negligible compared to the parallel component resistances. To get a voltage drop, you need current flowing through a resistance. V=IR, so if R is negligible, the V is too.

I also already answerd the second question. P/I=VI/I=V, which is the same for all branches.

Let's try the second one a different way to see if it helps. Let's say that you have a single resistor of value R across the power supply, so obviously I=V/R, and P=VI=V^2/R. Now split that resistor into two parallel resistors of value 2R each, so the total I=V/R still, but now I/2 flows through 2R in each of the two parallel branches. Do you see where I'm going with this? What do you do next in this exercise to show the property that you are asking about? What is the current in each of the 2 parallel legs? What is the power in each of the two split legs compared to the original power in the single R before the split? Does that make it more intuitive?

Yes I get what you are trying to explain. But aren't we following a circular argument since we try to explain with equations, which are derived from certain concepts?

I just can't seem to understand why is the voltage drop across each resistor
the same? Why can't it be different? We argue that voltage drops because of resistance, but in parallel component, why must the drop be the same?

@Frogpad: Yea this explanation is what most of my teachers use when I was taught a few years back. But it seems that I'm still stucked at the problem with why can't the 'pressure' be different in the parallel component.

Thanks everyone for your replies but it seems that my brain has become 'more retarded'.
 
  • #14
truewt said:
Yes I get what you are trying to explain. But aren't we following a circular argument since we try to explain with equations, which are derived from certain concepts?

I just can't seem to understand why is the voltage drop across each resistor
the same? Why can't it be different? We argue that voltage drops because of resistance, but in parallel component, why must the drop be the same?

@Frogpad: Yea this explanation is what most of my teachers use when I was taught a few years back. But it seems that I'm still stucked at the problem with why can't the 'pressure' be different in the parallel component.

Thanks everyone for your replies but it seems that my brain has become 'more retarded'.

The pressure is the same, but the RATE at which the water is flowing is different.

Maybe we can think of it like this (this is not a 100% accurate analogy).

When you hook up one pipe there is water moving through. Imagine it moving really fast through the pipe.

Now when you hook up two pipes, the water is now split, so the flow must decrease accordingly in each pipe. Imagine the water slowing down in each of these pipes.

Now hook up 10 pipes. What would happen to the flow of water?

But the thing is, this whole time the PRESSURE on the top of these pipes has remained constant. You are applying the pressure to the top equally. Imagine this:

if you stand on a board with a spring underneath.
like
____________
[___________]
-------S
-------S
-------S
______S______

If S is the spring and you are standing on the board on the top you put a certain amount of force on the BOARD right?

Now imagine putting two springs underneath. When you stand on the board you put the same amount of force on the board right? Your weight hasn't changed. However, the system underneath has. Try to mentally think about the difference between current and voltage.

At least for me, I may not have a 100% correct mental image, but I have intuition from these models. Now back your intuition up with the math.

Maybe it would serve better to explain at an atomic level what is going on?
 
  • #15
The following explanation assumes this experimental setup: Two resistors of unequal resistance R1 and R2 connected in parallel to a constant DC emf source. Let the current through R1 and R2 be I1 and I2. And pds across each of them be V1 and V2. U denotes the energy dissipated by the entire circuit in a given time t. U1 and U2 denotes the energy disspiated in R1 and R2 over the same time t.

We know that V = U/q right? Now we show that U = VIt . For a constant current, q = It. Hence U = VIt.

Now we make use of the principle of conservation of energy. This is essentially the explanation why pds across parallel circuits are the same.

You would agree that the energy dissipated by the entire circuit in a given time t would be equivalent to the sum of the energy disspated by both R1 and R2, right?

Hence U = U1 + U2, for a given time t.

VIt = V1(I1)t + V2(I2)t

Since by Kirchoff's current law, I = I2 + I1 (may be proven by conservation of charge),

V(I1 + I2)t = V1(I1)t + V2(I2)t

Dividing by t:

V(I1) + V(I2) = V1(I1) + V2(I2),

where by comparing coefficients, we see that the only way the above is true is when V=V1=V2.

Hope this helps.
 
  • #16
Thanks Defennnder, now I have come up with a very mathematical proof for what you mentioned. Some arguments involved which you fail to mention. But thanks for giving me a lead.

Anyhow, I still find it fascinating that charges are so smart as to be able to use the same amount of energy supplied to each individual charge to overcome the resistance when the circuit is set up in parallel branches.

And the same goes for the water pressure system. In parallel pipes (Frogpad's illustration), the water is able to maintain the same pressure under the correct circumstance (cross sectional area of pipe) after passing through the resistance. Or is it more correct to say that we are forcing the water pressure to remain constant by setting up the pipes to certain measurements?

Because from the water pipe analogy, I found out that in order for the water pressure to be the same in both parallel pipes after passing through the resistance, you need to 'configure' the pipe's cross sectional area in order to allow for that. Or am I wrong?
 
  • #17
truewt said:
Anyhow, I still find it fascinating that charges are so smart as to be able to use the same amount of energy supplied to each individual charge to overcome the resistance when the circuit is set up in parallel branches.

Charges do what they do. Why do they do things that follow any order at all? Why have they followed the same order for every experiment for a couple hundred years? Why can't we trick them? It is fascinating.

If you are looking for a answer that doesn't use math I would suggest finding a book about the history of science or a history of the early scientists. It is very likely your library would have a good one.

Look for something that reads similar to http://en.wikipedia.org/wiki/Georg_Ohm#_note-1

This will probably put charges into a different context for you to think about them. And should aid in figuring out why charges are so smart.
 
  • #18
truewt said:
Thanks Defennnder, now I have come up with a very mathematical proof for what you mentioned. Some arguments involved which you fail to mention. But thanks for giving me a lead.

Anyhow, I still find it fascinating that charges are so smart as to be able to use the same amount of energy supplied to each individual charge to overcome the resistance when the circuit is set up in parallel branches.

And the same goes for the water pressure system. In parallel pipes (Frogpad's illustration), the water is able to maintain the same pressure under the correct circumstance (cross sectional area of pipe) after passing through the resistance. Or is it more correct to say that we are forcing the water pressure to remain constant by setting up the pipes to certain measurements?

Because from the water pipe analogy, I found out that in order for the water pressure to be the same in both parallel pipes after passing through the resistance, you need to 'configure' the pipe's cross sectional area in order to allow for that. Or am I wrong?

If I put my hand on your back and push, why doesn't my hand go through your body? You could argue philosophy, or maybe argue from an atomic standpoint. Let's pick the atomic standpoint and dramatically simplify the situation. Consider two protons atoms. One proton can represent my hand, the other your back. Let's completely disregard quantum effects. As I move two protons together a Coulombic force will exist between them; opposites attract, and likes' repel. Do you accept this?

From your argument, you should not. Why are the protons smart enough to obey Coulombs law? In fact why does any artifact of nature obey physical laws? I think a better way of phrasing it would to say, why do OUR models of the natural world characterize these systems so well? As you can see, these questions quickly digress, but I hope you see my point.

The resistance of a nearly uniform current density inside a conductor can be modeled as:

[tex] R = \frac{\rho L}{A} [/tex]
Where A is the cross section of the conductor, L is the length of the conductor, and [itex] \rho [/itex] is the resistivity.

Notice the dependence on cross section though. When you increase the cross section, you decrease the resistance.

About the water analogy. You MUST remember that this is a CLOSED system! You can add all these pipes to our imaginary system, but in the end they all connect to one point, and end at one point (since they are in parallel). So when thinking of a potential difference, it is the the potential difference across the top and bottom of all the pipes.
 
  • #19
Thanks Frogpad. I get where you're going.

Talking about the two protons analogy you gave, coulombs' law is a hypothesis proven theory later on for an observation made? What about this parallel circuit issue? Was the 'law' a hypothesis proven theory after an observation was made first?

I can't understand the explanation you gave for the water analogy. Right now I think I'm digressing the topic, because my mind is some sort thinking more deeply into the water system instead of the water pipe system as an analogy for the electrical system.

Because we know water pressure is dependent on the speed of the water, and the speed of the water is dependent on the flow rate which in turn is dependent on the cross sectional area of the pipes.

That is why I am sort of thinking that in order to use the water pipe system as an analogy, we sort of need to configure the variables.
 
  • #20
truewt said:
Thanks Frogpad. I get where you're going.

Talking about the two protons analogy you gave, coulombs' law is a hypothesis proven theory later on for an observation made? What about this parallel circuit issue? Was the 'law' a hypothesis proven theory after an observation was made first?

I can't understand the explanation you gave for the water analogy. Right now I think I'm digressing the topic, because my mind is some sort thinking more deeply into the water system instead of the water pipe system as an analogy for the electrical system.

Because we know water pressure is dependent on the speed of the water, and the speed of the water is dependent on the flow rate which in turn is dependent on the cross sectional area of the pipes.

That is why I am sort of thinking that in order to use the water pipe system as an analogy, we sort of need to configure the variables.


What math class are you up to?
What physics (or engineering class) are you up to?

The reason I ask, is I think you will be unsatisfied with an anwer until you take more uppder division classes. It would not be a such a bad idea to just accept that the potential across a parallel circuit is the same in the ideal case. I mean you are definitely NOT denying it. So first accept this as fact, and then keep asking questions. Just so you know, I am not trying to jump ship. You can keep this thread open until you die. Someone WILL be able to answer your question in a suitable fashion.

About the water analogy. Honestly, I only use that analogy to gain intution into the problem. I don't know if they map 1:1 (so to speak). When I get some time, I will look into water pressure and see how much that relates to your question.



truewt said:
Was the 'law' a hypothesis proven theory after an observation was made first?
I think I see more where you are coming from with this statement. I honestly don't know. All I can say is it just makes sense inuitively for me. I don't know if it did early in my studies or not; I guess I have blocked that out.

Answer the first two questions I asked in this thread. We can always go the route of jumping into it from a more rigorous (as rigourous as I can make it anyways (don't count on much)) treatement of what you are asking by jumping into it from a vector analysis approach.
 
  • #21
Oh currently I've ceased my studies, but my highest qualification would be GCE A Levels.

I wouldn't say I have not accepted the fact that across parallel circuits, the potential difference is equal. It is an observation that I've seen myself in labs, and I know it IS a fact, but here I'm actually looking for an explanation that can be accepted by me.

What was the first two questions that you asked? I looked through the past posts but couldn't find it, but instead, I "found" more questions to ask.

In your previous post, you mentioned that in the water pipe analogy, the flow of the water DECREASES as the pipe splits into 2 different branches. However, I beg to differ that. Because what I found is that, the MASS FLOW rate decreases, but flow cannot decrease (flow as in speed of water flow) as the water pressure is dependent on the water flow rate. By Bernouli's principle of course.

Or am I wrong to claim that?
 
  • #22
truewt said:
Oh currently I've ceased my studies, but my highest qualification would be GCE A Levels.

I wouldn't say I have not accepted the fact that across parallel circuits, the potential difference is equal. It is an observation that I've seen myself in labs, and I know it IS a fact, but here I'm actually looking for an explanation that can be accepted by me.

What was the first two questions that you asked? I looked through the past posts but couldn't find it, but instead, I "found" more questions to ask.

In your previous post, you mentioned that in the water pipe analogy, the flow of the water DECREASES as the pipe splits into 2 different branches. However, I beg to differ that. Because what I found is that, the MASS FLOW rate decreases, but flow cannot decrease (flow as in speed of water flow) as the water pressure is dependent on the water flow rate. By Bernouli's principle of course.

Or am I wrong to claim that?


Like I said, I use that analogy only for intuition. I would say you are correct in saying that the MASS FLOW rate decreases.

This makes sense with current right?
[tex] I = \frac{Q}{T} [/tex]

Where [itex] Q [/itex] is the amount of charge at time T. So if you have two pipes, the charges will be distributed.

The questions I was referring to were:
1) What math class are you up to?
2) What physics (or engineering class) are you up to?

Yeah man. I was saying that you HAVE accepted it as fact. I am just saying it may be better to just accept it, and then move on. I highly recommend the book:
"Field and wave Electromagnetics" by Cheng.

If you went through that book, it would be very helpful. It takes awhile though.

Are you comfortable with vectors, and vector notation? I'm not sure what GCE A Levels is, as I am from the states.
 
  • #23
truewt said:
I am currently having some difficulty in recalling/understanding the potential difference across parallel circuits. Why is the potential difference across individual components of the parallel circuit the same?
I find it helpful to think of voltage as being analogous to altitude. Think about two points on the Earth's surface, say the top of Mount Everest and Tower of London. There are multiple paths we can travel from Mount Everest to the Tower of London, but each path results in the same drop in altitude. We can take this analogy one step further and equate altitude to gravitational potential energy.

In the same way, any given point in a circuit can only have one value for electrical potential, (just as any given point, on the Earths surface can have only one altitude). Therefore the potential difference between any two given points can only have one value.

Claude.
 
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  • #24
FrogPad said:
Like I said, I use that analogy only for intuition. I would say you are correct in saying that the MASS FLOW rate decreases.

This makes sense with current right?
[tex] I = \frac{Q}{T} [/tex]

Where [itex] Q [/itex] is the amount of charge at time T. So if you have two pipes, the charges will be distributed.

The questions I was referring to were:
1) What math class are you up to?
2) What physics (or engineering class) are you up to?

Yeah man. I was saying that you HAVE accepted it as fact. I am just saying it may be better to just accept it, and then move on. I highly recommend the book:
"Field and wave Electromagnetics" by Cheng.

If you went through that book, it would be very helpful. It takes awhile though.

Are you comfortable with vectors, and vector notation? I'm not sure what GCE A Levels is, as I am from the states.

Yes I do understand the point with charges being splitted as they branch out. What I'm uncomfortable with is the potentials.

GCE A Level is a pre-university exam. College exam for entrance to university, if you'd call it. My country follows the british educational system, so I'm not too sure which grade it is equivalent to the states.

Claude Bile said:
I find it helpful to think of voltage as being analogous to altitude. Think about two points on the Earth's surface, say the top of Mount Everest and Tower of London. There are multiple paths we can travel from Mount Everest to the Tower of London, but each path results in the same drop in altitude. We can take this analogy one step further and equate altitude to gravitational potential energy.

In the same way, any given point in a circuit can only have one value for electrical potential, (just as any given point, on the Earths surface can have only one altitude). Therefore the potential difference between any two given points can only have one value.

Claude.

Yes this analogy can be accepted by me. No problem. But if you would put resistors into the paths along the altitudes, again I will have trouble becoming comfortable with the analogy.

For example, down a mountain, we come across a junction (from a path). The GPE at a certain altitude is fixed, no matter which path we are talking about. But we have to bring in the point in that the loss in GPE is used to do some work (as in the case of current,voltage and resistance). When you bring it in, there will be conflicts again.
 
  • #25
truewt said:
But we have to bring in the point in that the loss in GPE is used to do some work (as in the case of current,voltage and resistance). When you bring it in, there will be conflicts again.
Where are the conflicts? A loss in GPE is a loss in altitude period. Full stop. How that lost energy is used is irrelevant. Same with an electrical circuit.

Consider the converse case, that potential IS dependent on the path taken. Then you could give the SAME point in space TWO different values for potential energy. This is not just impossible, it is nonsensical.

Claude.
 
  • #26
My entire argument is regarding the energy lost as current passes through the resistor. Hence, my conflict here is that the GPE lost as you descend the mountain, where is it going?

I get where you are going. As long as the points are connected without any resistances inbetween the connections, the potential will be the same. Hence, in the parallel branch, as long as we move from point A to point B with resistances inbetween, energy loss per unit charge will be the same, regardless of the resistances in branch 1 or 2.
 
  • #27
truewt said:
My entire argument is regarding the energy lost as current passes through the resistor. Hence, my conflict here is that the GPE lost as you descend the mountain, where is it going?
It doesn't matter, it is lost, it is not conserved. Kinetic energy, heat, powering a toy car, doesn't matter. It's like getting worried about whether the energy stored in a battery is being used to drive a heater, a light bulb or a refrigerator.
truewt said:
Hence, in the parallel branch, as long as we move from point A to point B with resistances inbetween, energy loss per unit charge will be the same, regardless of the resistances in branch 1 or 2.
Yes. Again, where the lost energy goes is irrelevant in terms of circuit operation.

Claude.
 
  • #28
Claude Bile said:
It doesn't matter, it is lost, it is not conserved. Kinetic energy, heat, powering a toy car, doesn't matter. It's like getting worried about whether the energy stored in a battery is being used to drive a heater, a light bulb or a refrigerator.

Yes. Again, where the lost energy goes is irrelevant in terms of circuit operation.

Claude.


Right. But your explanation can't convince me. What it does is to tell me to accept it as a fact.

What I am concern is the resistance on both paths, when they are different, the amount of energy lost is still the same. Why is that so?
 
  • #29
truewt - I'm joining this discussion a little late, but maybe I can still help to clear up some of your confusion.

I think you're leading yourself astray in the way you're thinking about the definition of electrical potential. Yes, it is defined to be the work required to move a charge from point A to point B, but that definition applies to the work that was needed to establish the potential difference in the first place. You presumably have some voltage source connected to your circuit, let's say a battery, so the voltage represents the work the battery does when it "lifts" charges from the lower potential at its negative terminal to the higher potential ( or altitude, I like that analogy as well) at the positive terminal. I tend to think about these kinds of circuits like roller coaster rides, where the battery is the mechanism that lifts the cars to the highest point, and then they just roll "downhill" wherever there is a potential drop.

So ... the battery has a voltage between its terminals, defined as above, and that is unchanged no matter what resistance circuit is placed between them. Even if the terminals are disconnected (infinite resistance), the voltage is still there, unchanged. Now, when you put your parallel circuit between the terminals, you're still measuring the potential difference between the same two points, so it must be the same. If you had different voltage drops across the two resistors, then you'd have to have a potential difference between two connected ends of the resistors, but since they're connected only by ideal wire, you'd get an infinite current there - can't be.

You're correct that there's a different amount of work being done as charges traverse each of the two resistors, but that just means that different amounts of energy are being dissipated from the resistors (one gets hotter). It's like you have kids sliding down two sliding boards of equal height, but one has greater friction. The kids going down that board will slide more slowly, hence fewer of them will go down per minute, and their butts will get hotter. The change in their potential energy from top to bottom is the same, however.

Did that help any?
- Bruce
 
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  • #30
belliott4488 said:
truewt - I'm joining this discussion a little late, but maybe I can still help to clear up some of your confusion.

I think you're leading yourself astray in the way you're thinking about the definition of electrical potential. Yes, it is defined to be the work required to move a charge from point A to point B, but that definition applies to the work that was needed to establish the potential difference in the first place. You presumably have some voltage source connected to your circuit, let's say a battery, so the voltage represents the work the battery does when it "lifts" charges from the lower potential at its negative terminal to the higher potential ( or altitude, I like that analogy as well) at the positive terminal. I tend to think about these kinds of circuits like roller coaster rides, where the battery is the mechanism that lifts the cars to the highest point, and then they just roll "downhill" wherever there is a potential drop.

So ... the battery has a voltage between its terminals, defined as above, and that is unchanged no matter what resistance circuit is placed between them. Even if the terminals are disconnected (infinite resistance), the voltage is still there, unchanged. Now, when you put your parallel circuit between the terminals, you're still measuring the potential difference between the same two points, so it must be the same. If you had different voltage drops across the two resistors, then you'd have to have a potential difference between two connected ends of the resistors, but since they're connected only by ideal wire, you'd get an infinite current there - can't be.

You're correct that there's a different amount of work being done as charges traverse each of the two resistors, but that just means that different amounts of energy are being dissipated from the resistors (one gets hotter). It's like you have kids sliding down two sliding boards of equal height, but one has greater friction. The kids going down that board will slide more slowly, hence fewer of them will go down per minute, and their butts will get hotter. The change in their potential energy from top to bottom is the same, however.

Did that help any?
- Bruce

Thank you Bruce. I understand your point here.

So my mistake to begin with is, that electrical potential takes precedence first, hence we see the same potential difference across a parallel circuit (and their components). So my argument is somewhat incorrect to begin with as I had an incorrect starting point to my argument.

Thanks for clearing that up :)

And oh, the lower the resistance, the higher the amount of energy dissipated (in the parallel circuit). Am I right to say that?

For the water analogy, is there somewhat a problem with the analogy given? As in the pre-requisites for the water pipes in order for the water pressures to be applicable (applicable as an analogy) for the electric circuit problem?
 
  • #31
truewt said:
Thank you Bruce. I understand your point here.

So my mistake to begin with is, that electrical potential takes precedence first, hence we see the same potential difference across a parallel circuit (and their components). So my argument is somewhat incorrect to begin with as I had an incorrect starting point to my argument.

Thanks for clearing that up :)
No problem. I think you've got it now.
truewt said:
And oh, the lower the resistance, the higher the amount of energy dissipated (in the parallel circuit). Am I right to say that?
Oops - yeah, I think I might have misstated that. Lower resistance -> higher current -> greater power dissipation. I got thrown off by my friction analogy.:uhh:

truewt said:
For the water analogy, is there somewhat a problem with the analogy given? As in the pre-requisites for the water pipes in order for the water pressures to be applicable (applicable as an analogy) for the electric circuit problem?
I'll have to let someone else answer that ... I'm not a big fan of the water analogy, despite its common use for problems like this.
- Bruce
 
  • #32
belliott4488 said:
No problem. I think you've got it now.

Oops - yeah, I think I might have misstated that. Lower resistance -> higher current -> greater power dissipation. I got thrown off by my friction analogy.:uhh:


I'll have to let someone else answer that ... I'm not a big fan of the water analogy, despite its common use for problems like this.
- Bruce

Ahhh. I don't think you gave me a wrong impression. But its just that the lower the resistance, its only intuitive that the power dissipated is smaller. But its not the case in parallel circuits
 
  • #33
truewt said:
Ahhh. I don't think you gave me a wrong impression. But its just that the lower the resistance, its only intuitive that the power dissipated is smaller. But its not the case in parallel circuits

Found a good link for yah... http://hyperphysics.phy-astr.gsu.edu/hbase/electric/watcir.html

click on components of the DC circuit
 
  • #34
truewt said:
Ahhh. I don't think you gave me a wrong impression. But its just that the lower the resistance, its only intuitive that the power dissipated is smaller. But its not the case in parallel circuits
Wait a minute! That's what's wrong. :eek: Lower resistance -> more current -> MORE power dissipated!

This is something I used to get backwards, until I got my intuition fixed. A larger resistance does NOT present a larger load to a voltage source, despite what you'd think based on the wording. This is clear if you just think in extremes - an open circuit presents an infinite resistance but no load at all, whereas a short-circuit presents zero resistance and generally fries things (too high a load).
 
  • #35
Thank you Frogpad. That analogy helped, but there are still points that I'm still unsure of.

We're taking potential energy into account? What about Bernouli's principle, where the pressure changes due to the change in water flow rate? The flow rate is changing throughout its flow, am I right?
 

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