Circuit using maths and electricity laws/formulae

In summary, the conversation is about a circuit problem where the task is to solve for the currents i1 to i8 in terms of V and R using Kirchoff's current law and Ohm's law. The conversation includes discussions of using unknown voltages, symmetry in the circuit, and the convention for current flow. It is suggested to use simple parallel/series combinations to solve the problem, and it is noted that the current flowing from D to E must be equal to the current from E to A. The question is then raised about the current flowing from B to E being equal to E to C.
  • #1
SteliosVas
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0

Homework Statement



Okay so we are given this circuit. I do not want to be told step by step what the answer (or worked solution is) but I am wanting some guidance about how I can start/continue on from what is given to us.

We obviously need a understanding of Kirchoff's current law.

Our task is to construct the remaining equations and then solve for the currents i1 to i8 in terms of V and R.

Homework Equations



Okay so I know Kirchoff's current law that says that there is a conservation of charge. that is if there is only two wires one has current going in, the other equal going out. So the sum of all currents at node = 0A, and total charge in closed loop is zero. Also know Ohm's law is V=IR.

The Attempt at a Solution


[/B]
With that in mind we know:

0=i1+i2+i3+i4

and V=i6R+i7R+i8R

We can for instance combine the left triangle which has R and 2R and 2R all in parallel which should give us ((1/R) + (1/2R) + (1/2R) ) -1? Am i heading down the right path? And since that all combines to be one resistor that is parallel to the bottom left triangle which has a R and 2R again?

and so on and so forth? How do I do the current? Could it be like i2+i6=i7?

Thanks a lot!
 

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  • #2
Have you thought of using unkown voltages instead ? You would only need three variables then .
 
  • #3
Qwertywerty said:
Have you thought of using unkown voltages instead ? You would only need three variables then .

What do you mean? No I didn't think of it at all? Could you explain?
 
  • #4
SteliosVas said:
What do you mean? No I didn't think of it at all? Could you explain?
Could you by any chance label the junctions ? It is going to be a bit difficult to explain without it .
 
  • #5
Qwertywerty said:
Could you by any chance label the junctions ? It is going to be a bit difficult to explain without it .
You mean like this?
 

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  • #6
Yes , that's better . Now , let potential at A be zero , and V at D .

You will have three unknown voltages - V1 , say , at E , V2 at B , and V3 at C .
Now write junction law at E , B and C , using voltages and resistances . You thus have three equations , three variables . Solve and find the variables' values .

Can you now write each individual current ?

Hope this helps .
 
  • #7
@SteliosVas ,

Use symmetry to simplify the circuit.
ss-png.86935.png


ss2-jpg.86936.jpg
 
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  • #8
What do you mean by symmetry? Sorry I do civil engineering not really too fond on electrical associated stuff.

So do you mean look at the left hand side of the circuit and than take the same for right? But doesn't it matter that the top right branch has a voltage source?
 
  • #9
Bump!
 
  • #10
The circuit is symmetric about a line that goes through the middle of the voltage source, the middle of the circuit, and the middle of the resistance with i7 flowing through it. If you divide the voltage source in 2 voltage sources in series, both with potential difference V/2, and the resistor into two resistances R/2 in series, the 3 points on the symmetry axis all must have the same potential, If you connect them with wires, the rest of the circuit can be quickly solved with the rules for series and parallel resistors.
 
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  • #11
Do you mean something like this?
 

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  • #12
SteliosVas said:
Do you mean something like this?
snapshot-jpg.87407.jpg


Yes, something like that.

You left out the 2R resistor between points E and C.

However, it's not two separate circuits the way you described it. If you split it that way neither part would be a circuit.Here's a different question to clarify what convention you may be using regarding current.

Which convention do you use for the direction of current flow?
A: Is it "conventional current" in which current is considered to be due to the flow of positive charge? It tends to flow in the circuit from the positive terminal of the voltage source to the negative terminal.

B: Is it "electron current" in which current is considered to be due to the flow of negatively charged electrons?​
 
  • #13
SammyS said:
snapshot-jpg.87407.jpg


Yes, something like that.

You left out the 2R resistor between points E and C.

However, it's not two separate circuits the way you described it. If you split it that way neither part would be a circuit.Here's a different question to clarify what convention you may be using regarding current.

Which convention do you use for the direction of current flow?
A: Is it "conventional current" in which current is considered to be due to the flow of positive charge? It tends to flow in the circuit from the positive terminal of the voltage source to the negative terminal.

B: Is it "electron current" in which current is considered to be due to the flow of negatively charged electrons?​
Okay well I would consider conventional current, that is it flows out of the positive terminal and than back into the negative...

But I am still not sure, could I use matricies for this problem?
 
  • #14
SteliosVas said:
Okay well I would consider conventional current, that is it flows out of the positive terminal and than back into the negative...

But I am still not sure, could I use matrices for this problem?
Yes, you could use matrices to solve this, but they are not needed.

The solution can be worked out with some simple parallel/series combinations.

Can you see that the current flowing from D to E must be equal to the current from E to A?
 
  • #15
SammyS said:
Yes, you could use matrices to solve this, but they are not needed.

The solution can be worked out with some simple parallel/series combinations.

Can you see that the current flowing from D to E must be equal to the current from E to A?
Yes I understand that cause the value of the resistor is the same?

Okay so my understanding is this. Since the current flowing through D to E = E to A
Does that imply say that the current flowing from B to E is equal to E to C

Or did you say the flow because what ever is entering junction E from the right is exiting from the top?

Than B to C is parallel to C to D ?

I sort of understand that you can combine together. So you can treat that top right hand corner as a circuit in series with say the top left? But parallel to the bottom two?

Edit:
Okay so it asks to come up with the remaining equations for i1 to i8

Would I be wrong in saying the first two are?
2Ri1+2Ri2+2Ri3+2Ri4 = V

Making i1+... i4=V/2R

The second being:

Ri6+2Ri2-Ri7=V?
 
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  • #16
SteliosVas said:
Yes I understand that cause the value of the resistor is the same?

Okay so my understanding is this. Since the current flowing through D to E = E to A
Does that imply say that the current flowing from B to E is equal to E to C
One does imply the other, but they're both true because of the symmetry in the circuit.

Or did you say the flow because what ever is entering junction E from the right is exiting from the top?
This is not not enough reason to imply those equalities.

Than Then B to C is parallel to C to D ?
No. That is definitely not true.

The rest is not correct.
I sort of understand that you can combine together. So you can treat that top right hand corner as a circuit in series with say the top left? But parallel to the bottom two?

Edit:
Okay so it asks to come up with the remaining equations for i1 to i8

Would I be wrong in saying the first two are?
2Ri1+2Ri2+2Ri3+2Ri4 = V

Making i1+... i4=V/2R

The second being:

Ri6+2Ri2-Ri7=V?

I didn't read willem2's post #10 carefully enough, previously.

That may be a simpler way to analyze this circuit.
 
  • #17
Okay analysing it your way. How should I start? It's more the beginning that is the most difficult.

If you draw a line across the voltage source therefore anything lying on that line must (I think equal =0) so saying that one resistor will have value R/2 and the junction E a value and v/2?

Using that should I than analyse the top and bottom segments ?
 
  • #18
SteliosVas said:
Okay analysing it your way. How should I start? It's more the beginning that is the most difficult.

If you draw a line across the voltage source therefore anything lying on that line must (I think equal =0) so saying that one resistor will have value R/2 and the junction E a value and v/2?

Using that should I than analyse the top and bottom segments ?
It is all the same voltage along that line. Maybe not zero.

At any rate, you can connect all along that line with a wire.

Which way do you want to analyze it?

The way willem2 suggests?
 
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  • #19
I guess it doesn't matter which way I analyse it. My understanding of series and parallel circuits and related laws.

What I don't understand is what is meant by symmetrical and I guess what throws me is the voltage source
 
  • #20
SteliosVas said:
I guess it doesn't matter which way I analyse it. My understanding of series and parallel circuits and related laws.

What I don't understand is what is meant by symmetrical and I guess what throws me is the voltage source
upload_2015-8-20_23-18-11.png


Does this help ?
 

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  • #21
SteliosVas said:
I guess it doesn't matter which way I analyse it. My understanding of series and parallel circuits and related laws.

What I don't understand is what is meant by symmetrical and I guess what throws me is the voltage source

Why don't you build the circuit using QUCs and see what is going on? You can probe parts of the circuit.
Then build the circuit Sammy suggests; then compare.
 
  • #22
William White said:
Why don't you build the circuit using QUCs and see what is going on? You can probe parts of the circuit.
Then build the circuit Sammy suggests; then compare.
What the heck is a QUC?

I doubt that using a circuit simulator will help OP understand how to analyze such a circuit.
 
  • #23
http://lmgtfy.com/?q=QUCs

I think a circuit simulator might help. Because you can add bits as you go, check the currents, add a bit more, see what has changed. I think it's exactly like building simple circuits at school: you'd add lightbulbs and measure currents to get an intuitive grasp of what is happening. Sometimes being able to build something and measure what is going on is better than struggling with the maths, and struggling with an abstract concept of what goes where, which seems to be happening here.
 
  • #24
William White said:
http://lmgtfy.com/?q=QUCs

I think a circuit simulator might help. Because you can add bits as you go, check the currents, add a bit more, see what has changed. I think it's exactly like building simple circuits at school: you'd add lightbulbs and measure currents to get an intuitive grasp of what is happening. Sometimes being able to build something and measure what is going on is better than struggling with the maths, and struggling with an abstract concept of what goes where, which seems to be happening here.
Good point.
 
  • #25
SteliosVas said:
I guess it doesn't matter which way I analyse it. My understanding of series and parallel circuits and related laws.

What I don't understand is what is meant by symmetrical and I guess what throws me is the voltage source
I would not have pursued "symmetry" quite as literally as the foregoing respondants.

Examining the pathways and resistor values, you can see that between point E and the top of the battery (i.e., the +V volts point) is exactly the same arrangement as between point E and the bottom of the battery (i.e., the 0 volts point). So, by symmetry, point E must be at a potential that is midway between +V and zero, meaning E must be V/2 volts.

ss2-jpg.86936.jpg


Back to the circuit, you can see that between node B and the top of the battery is the same arrangement as is seen between node C and the bottom of the battery. Consequently, if we say node B is x volts less than the potential at the top of the battery, then, its corresponding node under symmetry is going to be x volts more than the potential at the bottom of the battery.

So, this leaves us with only one unknown in the whole circuit, viz., x. Once we know x we'll know the voltage at every node and hence the voltage across every resistor.

➤ Apply Kirchoff's and Ohm's Laws to determine x.
 
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  • #26
William White said:
http://lmgtfy.com/?q=QUCs

I think a circuit simulator might help. Because you can add bits as you go, check the currents, add a bit more, see what has changed. I think it's exactly like building simple circuits at school: you'd add lightbulbs and measure currents to get an intuitive grasp of what is happening. Sometimes being able to build something and measure what is going on is better than struggling with the maths, and struggling with an abstract concept of what goes where, which seems to be happening here.

That is an idea, but I would like to understand what is going on before I start using simulators lol!
NascentOxygen said:
I would not have pursued "symmetry" quite as literally as the foregoing.

Examining the pathways and resistor values, you can see that between point E and the top of the battery (i.e., the +V volts point) is exactly the same arrangement as between point E and the bottom of the battery (i.e., the 0 volts point). So, by symmetry, point E must be at a potential that is midway between +V and zero, meaning E must be V/2 volts.

Back to the circuit, you can see that between node B and the top of the battery is the same arrangement as is seen between node C and the bottom of the battery. Consequently, if we say node B is x volts less than the potential at the top of the battery, then, its corresponding node under symmetry is going to be x volts more than the potential at the bottom of the battery.

So, this leaves us with only one unknown in the whole circuit, viz., x. Once we know x we'll know the voltage at every node and hence the voltage across every resistor.

➤ Apply Kirchoff's and Ohm's Laws to determine x.

Okay so my understanding is you are saying basically the branch between B and the top of the batter is the same as C and the battery because the value of the resistor is R.
Since the voltage at E is 1/2 the branch at top will be the potential at E - a certain difference and bottom will be E + the certain difference.
 
  • #27
SteliosVas said:
Okay so my understanding is you are saying basically the branch between B and the top of the battery is the same as C and the battery because the value of the resistor is R.
No, I didn't attribute it to any single resistor. There is a complicated arrangement of resistors between B and both terminals of the battery, and we can't easily simplify it. But whatever it is, we can see there is an identical/symmetrical arrangement positioned between C and the battery terminals. And that's all we need to know---that from both points B and C the resistor-battery arrangement is identical [in symmetry]. This allows us to state---without further ado---that the +V battery terminal and point B have the same voltage difference as that between point C and the 0 volts end of the battery.
 
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  • #28
NascentOxygen said:
No, I didn't attribute it to any single resistor. There is a complicated arrangement of resistors between B and both terminals of the battery, and we can't easily simplify it. But whatever it is, we can see there is an identical/symmetrical arrangement positioned between C and the battery terminals. And that's all we need to know---that from both points B and C the resistor-battery arrangement is identical [in symmetry]. This allows us to state---without further ado---that the +V battery terminal and point B have the same voltage difference as that between point C and the 0 volts end of the battery.

Thanks I eventually worked it out, I used a very hard way in the way of matrix but got it in the end

Thanks :)
 
  • #29
SteliosVas said:
Thanks I eventually worked it out, I used a very hard way in the way of matrix but got it in the end
But you will not always enjoy the luxury of being allowed to solve problems with symmetry using your "long way". These are favoured exam questions; they are solvable by all students, but only those who recognize the shortcuts of symmetry will reach the solution within the restricted time available in examinations.

I suggest that you attempt to solve it using the approach I outlined, for practice.
 

Related to Circuit using maths and electricity laws/formulae

1. What is Ohm's Law and how is it used in circuit analysis?

Ohm's Law states that the voltage across a resistor is directly proportional to the current flowing through it, and can be represented by the equation V=IR. This law is used in circuit analysis to calculate the voltage, current, or resistance in a circuit.

2. What is Kirchhoff's Voltage Law and how is it applied in circuit analysis?

Kirchhoff's Voltage Law states that the sum of all voltages around a closed loop in a circuit must equal zero. This law is applied in circuit analysis to determine the voltages at different points in a circuit and to check for any inconsistencies or errors in the circuit design.

3. How can I calculate the total resistance of resistors in series and parallel?

The total resistance of resistors in series can be calculated by simply adding the individual resistances together. In parallel, the total resistance can be calculated using the formula 1/Rt = 1/R1 + 1/R2 + ... + 1/Rn, where Rt is the total resistance and R1, R2, etc. are the individual resistances.

4. What is the difference between AC and DC circuits?

AC (alternating current) circuits have a continuously changing voltage and current, while DC (direct current) circuits have a constant voltage and current. AC circuits are commonly used for power transmission, while DC circuits are used in electronic devices such as batteries and computers.

5. How can I calculate the power and energy consumption in a circuit?

The power in a circuit can be calculated using the formula P=VI, where P is power, V is voltage, and I is current. The energy consumption can be calculated by multiplying the power by the time the circuit is in use, giving the unit watt-hours (Wh).

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