What is the equivalent resistance of this circuit?

In summary, the student is stuck on finding the equivalent resistance. They are unable to reduce the problem to simpler parallel and series combinations and are in need of help. The student has tried redrawing the circuits, labeling the nodes and resistors, and applying Kirchhoff's circuit laws but still cannot find a solution. They are considering posting a picture of their current thinking, and then selecting the loop that produces the equation V-xR-I2R=0.
  • #1
Saitama
4,243
93

Homework Statement


http://i50.tinypic.com/w0ggl.png

Homework Equations





The Attempt at a Solution


I am stuck at part (a) (i haven't yet tried the part (b)).
I really have no clue on how should i go on finding the equivalent resistance, i don't see a way to reduce it to simpler parallel and series combinations. Any help is appreciated.
 
Physics news on Phys.org
  • #2
Pranav-Arora said:

Homework Statement


http://i50.tinypic.com/w0ggl.png

Homework Equations



The Attempt at a Solution


I am stuck at part (a) (i haven't yet tried the part (b)).
I really have no clue on how should i go on finding the equivalent resistance, i don't see a way to reduce it to simpler parallel and series combinations. Any help is appreciated.
Try redrawing the circuits.

Label each node and resistor.
Use any symmetry you can find to your advantage.
 
Last edited:
  • #3
SammyS said:
Try redrawing the circuits.

Label each node and resistor.



Use any symmetry you can find to your advantage.

I see that i can apply delta star transformation, but i don't think it would be a good choice.
I don't see any symmetry here, can i have some hints?
 
  • #4
Are you aware of Kirchhoff's circuit laws?
 
  • #5
I like Serena said:
Are you aware of Kirchhoff's circuit laws?

Yes. :)
 
  • #6
Pranav-Arora said:
Yes. :)

So... did you apply them (making use of any symmetries that are apparent)?
 
  • #7
I like Serena said:
So... did you apply them (making use of any symmetries that are apparent)?

I thought of doing so but i cannot find the appropriate path.
And, still i don't see any symmetries. :(
 
  • #8
That's not much of an effort... yet. ;)
 
  • #9
I like Serena said:
That's not much of an effort... yet. ;)

Effort? I don't have an idea on how should i start. :)
I suppose i should post a pic of what i am thinking, the current in the resistors R1 and R2 should be the same as coming out of R3 and R4 due to symmetry, is that right?
 

Attachments

  • sym.png
    sym.png
    51.6 KB · Views: 443
  • #10
Through each resistor some unknown current Ik flows.
At each node between resistors you have some unknown Vk.

Some of those Ik might be the same due to symmetry.
Some of those Vk might be the same due to symmetry.

Set up a system of equations?
 
  • #11
I like Serena said:
Through each resistor some unknown current Ik flows.
At each node between resistors you have some unknown Vk.

Some of those Ik might be the same due to symmetry.
Some of those Vk might be the same due to symmetry.

Set up a system of equations?

I still don't get it. I can make the equation but i am not sure if i took the right use of symmetry. Can you review the attached pic? I have mentioned the current flowing through each resistor and took use of the symmetry of circuit, is it right?
 

Attachments

  • symc.png
    symc.png
    51.7 KB · Views: 471
  • #12
Your use of symmetry looks overall correct. :)

However, in your leftmost I2-I3 you seem to have ignored the current through the bottom most resistor?
 
  • #13
I like Serena said:
Your use of symmetry looks overall correct. :)

However, in your leftmost I2-I3 you seem to have ignored the current through the bottom most resistor?

Oops, sorry, i forgot about, i was focusing on the middle part. :P

I think i will have to again label the currents, i haven't sent any current in the topmost resistor too.
 
  • #14
Yeah well, if you designate the bottom current, the topmost one will be the same due to symmetry! :)
 
  • #15
I like Serena said:
Yeah well, if you designate the bottom current, the topmost one will be the same due to symmetry! :)

Yes, but i will have to reassign the currents to the diagonally placed resistor.
 
  • #16
Pranav-Arora said:
Yes, but i will have to reassign the currents to the diagonally placed resistor.

Yep.
 
  • #17
I like Serena said:
Yep.

Can you help me finding the right loop please? I have attached the figure with nodes marked.
I attached the battery. I could find one loop useful, AYHIJEBA, from here i get an equation,
V-xR-I2R=0, where x=I-I1-I2.
V=IR+I1R
Now which loop should i select? I am stuck here. :(

EDIT:Sorry, i forgot to mention I in the pic, its the current sent by the battery.
 

Attachments

  • symn.png
    symn.png
    49.1 KB · Views: 440
  • #18
That looks correct! :)

Why would you select a single loop?
Pick any loop you like.

For instance pick the one through the top.
The one through the bottom will be the same, so you can leave that one out.

Now keep picking loops until you have as much variables as you have equations (avoiding those that will duplicate existing equations).
 
  • #19
I like Serena said:
That looks correct! :)

Why would you select a single loop?
Pick any loop you like.

For instance pick the one through the top.
The one through the bottom will be the same, so you can leave that one out.

Now keep picking loops until you have as much variables as you have equations (avoiding those that will duplicate existing equations).

Thank you for all the help! :smile:
I think i can do it now, this is the worst question i have ever done on finding the equivalent resistance. Is their any easier way to do this? Any trick?
 
  • #20
Ah well, usually it starts looking as daunting.
And then you simply set up all equations using as many symmetries as you can.
And then it turns out you can solve it.
Afterwards, you'll see a couple of symmetries or some such that you missed.
But by then it doesn't matter anymore since you have the solution (assuming that you do).
 
  • #21
I like Serena said:
Ah well, usually it starts looking as daunting.
And then you simply set up all equations using as many symmetries as you can.
And then it turns out you can solve it.
Afterwards, you'll see a couple of symmetries or some such that you missed.
But by then it doesn't matter anymore since you have the solution (assuming that you do).

Most of the times i refrain myself from using the Kirchoff's laws to find the equivalent resistance. I never thought that i will have to use Kirchoff's laws here. I kind of get bored by making equations and selecting loops (I need to do that in my school exams as i can't use tricks in those exams. :-p ). I will see if i could find an alternative way to solve it.

Thanks once again! :smile:
 
  • #22
Let me know if you find an alternative solution! ;)

However, when you can't find equivalent resistances using regular parallel or series replacements, you will be stuck with Kirchhoff's laws.
 
  • #23
There is a trick: If you find two points in a circuit which are at the same potential you can connect them with a wire, so the two points become a single node.
See the attachment. When connecting a battery between A and B, both E and F are "at the middle" so at the same potential. connect E and F and fold the circuit so E and F become a single node: all pairs (A,F), (C,F), D,F), (B,F) are connected with two resistors in parallel. The orange lines represent R resistance, the blue represent R/2 resistance. The resistor in the middle can be halved, making a new node G. G is at the same potential as the node (EF). You can draw a short between G and (EF), and you have all parallel and series resistors between A and B at the end.

ehild
 

Attachments

  • transformations.JPG
    transformations.JPG
    17.4 KB · Views: 514
  • #24
attachment.php?attachmentid=49405&d=1343554966.jpg
Using what ehild gave you, now you can make use of Δ - Y transforms.

Change the ACE and BFD Δs to Ys & you can use series/parallel analysis !
 
  • #25
SammyS said:
Using what ehild gave you, now you can make use of Δ - Y transforms.

Change the ACE and BFD Δs to Ys & you can use series/parallel analysis !

It is not needed, Sammy. The node EF can be connected to point G and all resistors are either series of parallel.

(I hate Δ - Y transform:-p)

ehild.
 

Attachments

  • transformations2.JPG
    transformations2.JPG
    13.8 KB · Views: 389
  • #26
ehild said:
It is not needed, Sammy. The node EF can be connected to point G and all resistors are either series of parallel.

(I hate Δ - Y transform:-p)

ehild.
DUH !

Of course !

How did I not see that ?
 
  • #27
ehild said:
When connecting a battery between A and B, both E and F are "at the middle" so at the same potential.

Please explain this, i don't understand how you get this.
 
  • #28
Do you understand that the circuit in the first figure is equivalent with the second one?

You can consider a circuit as a graph. There are nodes connected by resistors, the resistors are equivalent by the edges of the graph.
Two graphs are equivalent if both have the same nodes, and the equivalent nodes are connected with the same number of edges.
The second figure is equivalent to the original circuit. (The orange lines represent the resistors)
The symmetry of the circuit is apparent in the second figure. The part left from the line EF is the mirror image of the part on the right. It is also symmetric to the line AB.
If you connect a battery between A and B the voltage drops the same from A to F as from A to E, and again the same from A to F and from F to B, from A to E and from E to B. E and F are at the same potential, and as both are "halfway" between A and B the potential difference VAF =VAE=VFB=VEB=VAB/2
Check your figure with the currents and voltages: You got the same situation.

ehild
 

Attachments

  • transform3.JPG
    transform3.JPG
    17.4 KB · Views: 351
  • #29
Pranav-Arora said:

Homework Statement


http://i50.tinypic.com/w0ggl.png

Homework Equations



The Attempt at a Solution


I am stuck at part (a) (i haven't yet tried the part (b)).
I really have no clue on how should i go on finding the equivalent resistance, i don't see a way to reduce it to simpler parallel and series combinations. Any help is appreciated.
Were you able to come up with a solution for circuit (b) ?
 
  • #30
I know its too late to reply to this thread now. I thought instead of creating a new thread, I will complete this one.

Thanks ehild, your trick was really helpful for the first question. :smile:

I gave a try to the second question but got stuck at the last step. The circuit is symmetrical about the line AB so I folded it and transformed it to as shown in the attachment. Now I am unable to proceed ahead. :(

EDIT: I have figured it out. It was easy once I applied the delta-Y transform. Thanks once again. :smile:
 

Attachments

  • resistors.jpg
    resistors.jpg
    7.3 KB · Views: 367
Last edited:
  • #31
Pranav-Arora said:
I know its too late to reply to this thread now. I thought instead of creating a new thread, I will complete this one.

Thanks ehild, your trick was really helpful for the first question. :smile:

I gave a try to the second question but got stuck at the last step. The circuit is symmetrical about the line AB so I folded it and transformed it to as shown in the attachment. Now I am unable to proceed ahead. :(

EDIT: I have figured it out. It was easy once I applied the delta-Y transform. Thanks once again. :smile:
Yes.

There is a Δ with three equal resistances. That's easy to convert to a Y .
 

FAQ: What is the equivalent resistance of this circuit?

What is the definition of equivalent resistance?

Equivalent resistance is the single resistance value that represents the combined effect of all resistors in a circuit. It is calculated using Ohm's Law, which states that resistance is equal to voltage divided by current.

How do you calculate the equivalent resistance of a series circuit?

In a series circuit, the equivalent resistance is equal to the sum of all individual resistances. This means you can simply add up all the resistance values to find the equivalent resistance.

How do you calculate the equivalent resistance of a parallel circuit?

In a parallel circuit, the equivalent resistance is calculated using the formula 1/Req = 1/R1 + 1/R2 + 1/R3 + ... + 1/Rn, where Req is the equivalent resistance and R1-Rn are the individual resistances. This means you need to find the reciprocal of each resistance, add them together, and then take the reciprocal of the sum to find the equivalent resistance.

What is the difference between series and parallel circuits in terms of equivalent resistance?

In a series circuit, the equivalent resistance is always greater than the individual resistances, while in a parallel circuit, the equivalent resistance is always less than the individual resistances. This is because in a series circuit, the current has to pass through each resistor, increasing the overall resistance, while in a parallel circuit, the current has multiple paths to take, decreasing the overall resistance.

Can the equivalent resistance of a circuit ever be negative?

No, the equivalent resistance of a circuit can never be negative. Resistance is a physical property that represents the hindrance to the flow of current, and it can never have a negative value. If you encounter a negative value when calculating equivalent resistance, it is likely due to an error in your calculations.

Similar threads

Back
Top