Circuit help - resistors and batteries in a network

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Homework Help Overview

The discussion revolves around analyzing a circuit with resistors and batteries, specifically focusing on calculating the current through each battery and the potential difference between two points in the circuit. The problem involves applying Kirchhoff's laws and understanding the relationships between currents and resistances in a network.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss setting up equations based on Kirchhoff's laws, with attempts to simplify and solve for currents in different loops of the circuit. There are questions about the correctness of signs in the equations and the relationships between the currents.

Discussion Status

Participants are actively revising their equations and discussing potential errors in their setups. Some guidance has been offered regarding checking the signs of terms and ensuring the correct application of Kirchhoff's laws. There is an ongoing exploration of the circuit's configuration and the implications of the assumed current directions.

Contextual Notes

Participants are working under the constraints of a homework assignment, which may limit the information they can use or the methods they can apply. There is an emphasis on ensuring the accuracy of their equations and understanding the underlying principles of circuit analysis.

lodovico
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circuit help -- resistors and batteries in a network

28_41.gif

Homework Statement



(a) Calculate the current through each ideal battery in Fig. 28-41.
(As a sign convention, assume the currents are "up" through each battery.)


A (I1)
A (I2)
A (I3)

Assume that R1 = 1.5 , R2 = 2.5 , ε1 = 2.0 V, and ε2 = ε3 = 3.5 V.

(b) Calculate Va - Vb



Homework Equations



V=iR


The Attempt at a Solution



I don't know how to approach this problem, use kirchhoffs law?
 
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Yes, Kirchhoff's laws or techniques based upon them are the way to go.
 


ok so i set up 3 loops and after simplifying i get:

Loop 1(the square on the left):-.6+1.2(i1)= i2
Loop 2(right square): 2.5(i2)=1.5(i3)
loop 3(the whole rectangle): 1.5=-3(i1+i2)

and that i1 = i2+i3
 


lodovico said:
ok so i set up 3 loops and after simplifying i get:

Loop 1(the square on the left):-.6+1.2(i1)= i2
Loop 2(right square): 2.5(i2)=1.5(i3)
loop 3(the whole rectangle): 1.5=-3(i1+i2)

and that i1 = i2+i3

Check the signs in your Loop 1 equation.

The coefficient of the i3 term in your Loop 2 equation doesn't look right.

Check the signs of the terms in your Loop 3 equation.
 


ok i just redid my loops I am not sure what is going wrong

1) 2-1.5(i1)-2.5(i2)-3.5-1.5(i1)=0
2) 3.5-2.5(i2)-1.5(i3)-3.5-1.5(i3)=0
3) 2-1.5(i1)-1.5(i3)-3.5-1.5(i3)-1.5(i1)=0

1) -.6-1.2(i1)=i2
2)-.833(i2)=i3
3)-.5-i3=i1
 


lodovico said:
ok i just redid my loops I am not sure what is going wrong

1) 2-1.5(i1)-2.5(i2)-3.5-1.5(i1)=0
2) 3.5-2.5(i2)-1.5(i3)-3.5-1.5(i3)=0
3) 2-1.5(i1)-1.5(i3)-3.5-1.5(i3)-1.5(i1)=0

1) -.6-1.2(i1)=i2
2)-.833(i2)=i3
3)-.5-i3=i1

Let's gather together the resistors in the branches and redraw the circuit showing the currents (blue) and the potential drops across the resistors (red) caused by those currents. This should make it easier to keep the signs of things straight when you do your "KVL walk" around a loop.
attachment.php?attachmentid=56105&stc=1&d=1361834650.gif


See if you can spot any sign issues in your equations.
 

Attachments

  • Fig2.gif
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1) -1.5-3(i1)-2.5(i2)=0
2) -2.5(i2)-3(i3)=0
3) -1.5-3(i1)-3(i3)=0

1) 1.5=-3(i1)-2.5(i2)
2)-2.5(i2)=3(i3)
3)1.5=-3(i1)-3(i3)
 


lodovico said:
1) -1.5-3(i1)-2.5(i2)=0
2) -2.5(i2)-3(i3)=0
3) -1.5-3(i1)-3(i3)=0

1) 1.5=-3(i1)-2.5(i2)
2)-2.5(i2)=3(i3)
3)1.5=-3(i1)-3(i3)

Did you pay attention to the directions of the potential changes on the resistors as you passed over them during your "walks" around the loops? I question the sign you've attributed to the 2.5(i2) term in your first loop equation, and to the 3(i3) terms in equations 2 and 3.

Remember, the polarities of the potential changes on the resistors are fixed by the assumed directions of the currents. You record those potential changes according to the direction you pass through the components as you proceed around the loop.
 

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