Finding the current and voltage for a resistor

AI Thread Summary
The discussion focuses on solving for the current and voltage across a resistor using Kirchhoff's Voltage Law (KVL) and Kirchhoff's Current Law (KCL). The user initially sets up equations based on loop currents but encounters difficulties with sign errors and complexity. Suggestions are made to simplify the problem by finding a linear combination of the equations to express all currents in terms of the same variable. Ultimately, the user concludes that to find the voltage across the resistor, they need to multiply the total current by the resistance value. The exchange highlights the importance of clarity in setting up equations and the potential for simplification in circuit analysis.
Davidllerenav
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Homework Statement
For the circuit in Figure 1, find the current and voltage at resistor R1 considering that the values of the voltage sources
they are V1 [V] and V2 [V], and the resistance values are R1 [Ω], R2 [Ω] and R3 [Ω] respectively.
Relevant Equations
Kirchhoff's Laws:
##\sum_i I_i=0##
##\sum_i V_i=0##
1573408396353.png

I tried to solve it by loop currents. So on the left mesh the loop current ##I_1## goes clockwise and on the right mesh the loop current ##I_2## goes counterclockwise.

1573409337462.png

I ended up with the following equations:
1) ##V_1-R_1(I_1+I_2)-R_2I_1=0##;
2) ##V_2-R_3I_2-R_1(I_1+I_2)=0##.
To find the current on ##R_1##, I tried to find ##I_1## and ##I_2##. I first solved 1) for ##I_1##: ##I_1=\frac{V_1-R_1I_2}{R_1+R_2}##. Then I solved 2) for ##I_2## replacing the expression that I found for ##I_1## :

##V_2-R_3I_2-R_1(I_1+I_2)=V_2-I_2(R_3-R_1)-R_1I_1##
##=V_2-I_2(R_3-R_1)-R_1\left(\frac{V_1-R_1I_2}{R_1+R_2}\right)=V_2-I_2(R_3-R_1)-R_1\left(\frac{V_1-R_1I_2}{R_1+R_2}\right)##
##=V_2(R_1+R_2)-I_2(R_3-R_1)(R_1+R_2)-R_1(V_1-R_1I_2)##
##=V_2(R_1+R_2)-I_2[(R_3-R_1)(R_1+R_2)-R_1^2]-R_1V_1##
##I_2=\frac{V_2(R_1+R_2)-R_1V_1}{(R_1+R_2)(R_3-R_1)-R_1^2}##​
Finally, I replaced ##I_2## on ##I_1##: ##I_1=\frac{V_1-R_1\left(\frac{V_2(R_1+R_2)-R_1V_1}{(R_1+R_2)(R_3-R_1)-R_1^2}\right)}{R_1+R_2}##. Am I correct?

I'm not sure how to find the voltage on ##R_1##, but I think that I need to find ##R_1(I_1+I_2)##, right?
 
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TBH, I never liked working problems with KVL. Can you try solving it with KCL instead? My KCL equations for this problem are a lot simpler than what you posted...
 
Davidllerenav said:
Homework Statement: For the circuit in Figure 1, find the current and voltage at resistor R1 considering that the values of the voltage sources
they are V1 [V] and V2 [V], and the resistance values are R1 [Ω], R2 [Ω] and R3 [Ω] respectively.
Homework Equations: Kirchhoff's Laws:
##\sum_i I_i=0##
##\sum_i V_i=0##

View attachment 252658
I tried to solve it by loop currents. So on the left mesh the loop current ##I_1## goes clockwise and on the right mesh the loop current ##I_2## goes counterclockwise.

View attachment 252659
I ended up with the following equations:
1) ##V_1-R_1(I_1+I_2)-R_2I_1=0##;
2) ##V_2-R_3I_2-R_1(I_1+I_2)=0##.
To find the current on ##R_1##, I tried to find ##I_1## and ##I_2##. I first solved 1) for ##I_1##: ##I_1=\frac{V_1-R_1I_2}{R_1+R_2}##. Then I solved 2) for ##I_2## replacing the expression that I found for ##I_1## :

##V_2-R_3I_2-R_1(I_1+I_2)=V_2-I_2(R_3-R_1)-R_1I_1##
##=V_2-I_2(R_3-R_1)-R_1\left(\frac{V_1-R_1I_2}{R_1+R_2}\right)=V_2-I_2(R_3-R_1)-R_1\left(\frac{V_1-R_1I_2}{R_1+R_2}\right)##
##=V_2(R_1+R_2)-I_2(R_3-R_1)(R_1+R_2)-R_1(V_1-R_1I_2)##
##=V_2(R_1+R_2)-I_2[(R_3-R_1)(R_1+R_2)-R_1^2]-R_1V_1##
##I_2=\frac{V_2(R_1+R_2)-R_1V_1}{(R_1+R_2)(R_3-R_1)-R_1^2}##​
Finally, I replaced ##I_2## on ##I_1##: ##I_1=\frac{V_1-R_1\left(\frac{V_2(R_1+R_2)-R_1V_1}{(R_1+R_2)(R_3-R_1)-R_1^2}\right)}{R_1+R_2}##. Am I correct?

I'm not sure how to find the voltage on ##R_1##, but I think that I need to find ##R_1(I_1+I_2)##, right?
You have a sign error in ##V_2-R_3I_2-R_1(I_1+I_2)=V_2-I_2(R_3-R_1)-R_1I_1##.
An easier way to proceed from (1) and (2) is to find a linear combination of them such that all references to currents are in the form ##I_1+I_2##.
 
berkeman said:
TBH, I never liked working problems with KVL. Can you try solving it with KCL instead? My KCL equations for this problem are a lot simpler than what you posted...
That would just change the ##I_1+I_2##, right? It would give an equation of ##I_1+I_2=I_3## I think.
 
haruspex said:
You have a sign error in ##V_2-R_3I_2-R_1(I_1+I_2)=V_2-I_2(R_3-R_1)-R_1I_1##.
An easier way to proceed from (1) and (2) is to find a linear combination of them such that all references to currents are in the form ##I_1+I_2##.
You're right, it would be ##V_2-R_3I_2-R_1(I_1+I_2)=V_2-I_2(R_3+R_1)-R_1I_1## , right?

How do I find a linear combination?
 
Last edited:
Davidllerenav said:
You're right, it would be ##V_2-R_3I_2-R_1(I_1+I_2)=V_2-I_2(R_3+R_1)-R_1I_1## , right?

How do I find a linear combination?
It just means multiplying each equation by some variable (different ones) and adding them.
In the equations, some terms are already in the form I1+I2, but in one you have an R2I1 and the other an R3I2. What two values do you need to multiply by so that both currents have the same coefficient?
 
haruspex said:
It just means multiplying each equation by some variable (different ones) and adding them.
In the equations, some terms are already in the form I1+I2, but in one you have an R2I1 and the other an R3I2. What two values do you need to multiply by so that both currents have the same coefficient?
##R_2I_2## would need to be multiplied by ##\left(\frac{1}{R_2}+\frac{I_2}{R_2I_1}\right)## and ##R_3I_2## by ##\left(\frac{1}{R_3}+\frac{I_1}{R_3I_2}\right)##, am I correct?
 
Davidllerenav said:
##R_2I_2## would need to be multiplied by ##\left(\frac{1}{R_2}+\frac{I_2}{R_2I_1}\right)## and ##R_3I_2## by ##\left(\frac{1}{R_3}+\frac{I_1}{R_3I_2}\right)##, am I correct?
You mean ##R_2I_1##, not ##R_2I_2##. But no, it's much simpler than that. A single variable in each case.
 
haruspex said:
You mean ##R_2I_1##, not ##R_2I_2##. But no, it's much simpler than that. A single variable in each case.
Yes, sorry for the typo. How would it be? Maybe ##R_3## and ##R_2##? then both would have ##R_2R_3##.
 
  • #10
Davidllerenav said:
Yes, sorry for the typo. How would it be? Maybe ##R_3## and ##R_2##? then both would have ##R_2R_3##.
Right. That should give you an equation from which you can find ##I_1+I_2## immediately.
 
  • #11
haruspex said:
Right. That should give you an equation from which you can find ##I_1+I_2## immediately.
Ok, then I would have:
##V_1R_3-R_1R_3(I_1+I_2)-R_2R_3I_1=0##
##V_2R_2-R_1R_2(I_1+I_2)-R_2R_3I_2=0##
Then I can subtract, right?
 
  • #12
Davidllerenav said:
Ok, then I would have:
##V_1R_3-R_1R_3(I_1+I_2)-R_2R_3I_1=0##
##V_2R_2-R_1R_2(I_1+I_2)-R_2R_3I_2=0##
Then I can subtract, right?
No, if you subtract you will have a term ##R_2R_3(I_1-I_2)##.
 
  • #13
haruspex said:
No, if you subtract you will have a term ##R_2R_3(I_1-I_2)##.
Then I'll add them, obtaining ##V_1R_3+V_2R_2-R_1R_3(I_1+I_2)-R_1R_2(I_1+I_2)-R_2R_3I_1-R_2R_3I_2=0## thus ##V_1R_3+V_2R_2-(I_1+I_2)[R_1R_3+R_1R_2]-R_2R_3(I1+I_2)=0##
##\Rightarrow V_1R_3+V_2R_2-(I_1+I_2)[R_1R_3+R_1R_2+R_2R_3]=0##. Am I correct?
 
  • #14
Davidllerenav said:
Then I'll add them, obtaining ##V_1R_3+V_2R_2-R_1R_3(I_1+I_2)-R_1R_2(I_1+I_2)-R_2R_3I_1-R_2R_3I_2=0## thus ##V_1R_3+V_2R_2-(I_1+I_2)[R_1R_3+R_1R_2]-R_2R_3(I1+I_2)=0##
##\Rightarrow V_1R_3+V_2R_2-(I_1+I_2)[R_1R_3+R_1R_2+R_2R_3]=0##. Am I correct?
That looks better.
 
  • #15
+I
haruspex said:
That looks better.
Then I only have to solve for ##I_1+I_2## and to find the voltage on ##R_1## I just multiply ##I_1+I_2## times ##R_1##, right?
 
  • #16
Davidllerenav said:
+I
Then I only have to solve for ##I_1+I_2## and to find the voltage on ##R_1## I just multiply ##I_1+I_2## times ##R_1##, right?
Yes.
 
  • #17
haruspex said:
Yes.
Thank you. I guess that if I continued simplifying my original expressions for ##I_1## and ##I_2## nd adding them I would arrive to the same answer, but this helped me a lot. Thanks!
 
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