3 batteries, 5 resistors using KCL & KVL

In summary: So, just keep plodding along. It will all come together eventually. If it helps, think of the sequence of steps like a dance routine. It's a series of steps in a sequence that you perform to get the desired result, just like a dance routine. And like a dance routine, you practice it over and over until you've got it down pat. And like a dance routine, you can use your scratch paper to write down the sequence of steps to help you remember them.In summary, the conversation discusses using Kirchhoff's Laws to find all the currents flowing in a circuit and determining the voltage across each resistor to show compliance with KVL. The equations used are KVL and KCL
  • #1
amy1983
7
0

Homework Statement



1. Using Kirchhoff’s Laws, find all the currents flowing in the circuit.

2. Hence, determine the voltage across each resistor and show that all loops comply with KVL


Homework Equations



KVL and KCL



The Attempt at a Solution



Please see the pictures attached
 

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  • #2
amy1983 said:

Homework Statement



1. Using Kirchhoff’s Laws, find all the currents flowing in the circuit.

2. Hence, determine the voltage across each resistor and show that all loops comply with KVL


Homework Equations



KVL and KCL



The Attempt at a Solution



Please see the pictures attached

Hi amy1983, Welcome to Physics Forums.

For your Loop 2 equation be careful about the orientation of the voltage sources; as you go around the loop in the direction of mesh current I2, both give potential rises.

Take another look at your Loop 3 equation. Again, pay attention to the voltage source polarity with respect to the current loop direction. Also check that you haven't inadvertently counted some voltage drops twice...
 
  • #3
It's a bit confusing because you've taken clockwise mesh currents as negative. Also that loop 2 is not correct. As Gneill said, you've made an error with values of the voltage sources in that loop.
 
  • #4
A good program to use for Nodal Analysis and Mesh Analysis is Pspice, for these kinds of circuits your answers can be checked very quickly.
 
  • #5
Hi gneill / NewtonianAlch - thank you kindly for your welcome and for your suggestions, I will review this PM.
 
  • #6
Hi g/neill / NewtonianAlch, I typed it all up and came up with the following according to your suggestions:

At node V_1,
I_1+I_2-I_3=0
⇒I_1+I_2=I_3
⇒(15-V_1)/(1 k)+(10-V_1)/(2 k)=(V_1-V_2)/(1 k)
⇒(30-2V_1 )+(10-V_1 )=(2V_1-2V_2)
⇒40-3V_1=2V_1-2V_2
⇒5V_1-2V_2=40
At node〖 V〗_2,
I_3-I_4-I_5=0
⇒I_3=I_4+I_5
⇒(V_1-V_2)/(1 k)=(5-V_2)/(1 k)+V_2/(2 k)
⇒2(V_1-V_2 )=(10-2V_2 )+V_2
⇒2V_1-V_2=10
Solving the two equations;
V_1=-20V &V_2=30V
I_1=(15-V_1)/(1 k)
⇒I_1=(15-(-20))/(1 k)
⇒I_1=35/(1 k)
⇒I_1=35mA
I_2=(10-V_1)/(2 k)
⇒I_2=(10-(-20))/(2 k)
⇒I_2=30/(2 k)
⇒I_2=15mA
I_3=(V_1-V_2)/(1 k)
⇒I_3=((-20)-30)/(1 k)
⇒I_3=(-50)/(1 k)
⇒I_3=-50mA
I_4=(5-V_2)/(1 k)
⇒I_4=(5-30)/(1 k)
⇒I_4=(-25)/(1 k)
⇒I_4=-25mA
I_5=V_2/(2 k)
⇒I_5=30/(2 k)
⇒I_5=15mA




Using KVL,
E_1-E_(R_1k )+E_(R_2k )-E_2=0
Where,
E_(R_1k )=I_1×R_1k
〖⇒E〗_(R_1k )=35×〖10〗^(-3)×1×〖10〗^3
〖⇒E〗_(R_1k )=35V

E_(R_2k )=I_2×R_2k
〖⇒E〗_(R_2k )=15×〖10〗^(-3)×2×〖10〗^3
〖⇒E〗_(R_2k )=30V
⇒E_1-E_(R_1k )+E_(R_2k )-E_2=0
⇒15-35+30-10=0
 
  • #7
amy1983 said:
Hi g/neill / NewtonianAlch, I typed it all up and came up with the following according to your suggestions:

At node V_1,
I_1+I_2-I_3=0
⇒I_1+I_2=I_3
⇒(15-V_1)/(1 k)+(10-V_1)/(2 k)=(V_1-V_2)/(1 k)
⇒(30-2V_1 )+(10-V_1 )=(2V_1-2V_2)
⇒40-3V_1=2V_1-2V_2
⇒5V_1-2V_2=40
Okay, looks good for Node V1.
At node〖 V〗_2,
I_3-I_4-I_5=0
⇒I_3=I_4+I_5
⇒(V_1-V_2)/(1 k)=(5-V_2)/(1 k)+V_2/(2 k)
Oops. Check the polarity of the E3 source. Is it going to make the potential difference across R4 larger or smaller?
⇒2(V_1-V_2 )=(10-2V_2 )+V_2
⇒2V_1-V_2=10
 
  • #8
At node V_1,
I_1+I_2-I_3=0
⇒I_1+I_2=I_3
⇒(15-V_1)/(1 k)+(10-V_1)/(2 k)=(V_1-V_2)/(1 k)
⇒(30-2V_1 )+(10-V_1 )=(2V_1-2V_2)
⇒40-3V_1=2V_1-2V_2
⇒5V_1-2V_2=40
At node〖 V〗_2,
I_3-I_4-I_5=0
⇒I_3=I_4+I_5
⇒(V_1-V_2)/(1 k)=(5+V_2)/(1 k)+V_2/(2 k)
⇒2(V_1-V_2 )=(10+2V_2 )+V_2
⇒2V_1-2V_2=10
Solving the two equations;
V_1=-20V &V_2=30V
I_1=(15-V_1)/(1 k)
⇒I_1=(15-(-20))/(1 k)
⇒I_1=35/(1 k)
⇒I_1=35mA
I_2=(10-V_1)/(2 k)
⇒I_2=(10-(-20))/(2 k)
⇒I_2=30/(2 k)
⇒I_2=15mA
I_3=(V_1-V_2)/(1 k)
⇒I_3=((-20)-30)/(1 k)
⇒I_3=(-50)/(1 k)
⇒I_3=-50mA
I_4=(5+V_2)/(1 k)
⇒I_4=(5+30)/(1 k)
⇒I_4=35/(1 k)
⇒I_4=35mA
I_5=V_2/(2 k)
⇒I_5=30/(2 k)
⇒I_5=15mA

Using KVL,
E_1-E_(R_1k )+E_(R_2k )-E_2=0
Where,
E_(R_1k )=I_1×R_1k
〖⇒E〗_(R_1k )=35×〖10〗^(-3)×1×〖10〗^3
〖⇒E〗_(R_1k )=35V

E_(R_2k )=I_2×R_2k
〖⇒E〗_(R_2k )=15×〖10〗^(-3)×2×〖10〗^3
〖⇒E〗_(R_2k )=30V
⇒E_1-E_(R_1k )+E_(R_2k )-E_2=0
⇒15-35+30-10=0
Hi gneill, Thank you for your advice. Does the remainder of the equation look okay?
 
  • #9
amy1983 said:
At node V_1,
I_1+I_2-I_3=0
⇒I_1+I_2=I_3
⇒(15-V_1)/(1 k)+(10-V_1)/(2 k)=(V_1-V_2)/(1 k)
⇒(30-2V_1 )+(10-V_1 )=(2V_1-2V_2)
⇒40-3V_1=2V_1-2V_2
⇒5V_1-2V_2=40
At node〖 V〗_2,
I_3-I_4-I_5=0
⇒I_3=I_4+I_5
⇒(V_1-V_2)/(1 k)=(5+V_2)/(1 k)+V_2/(2 k)
⇒2(V_1-V_2 )=(10+2V_2 )+V_2
⇒2V_1-2V_2=10
Oops again. I think you added the V_2's from the right hand side to the left hand side rather than subtracting them from both sides. But you're getting there...
 
  • #10
I_3-I_4-I_5=0
⇒I_3=I_4+I_5
⇒(V_1-V_2)/(1 k)=(5+V_2)/(1 k)+V_2/(2 k)
⇒2(V_1-V_2 )=(10+2V_2 )+V_2
⇒2V_1-2V_2=10V_2+2V_2
⇒2V_1=10V_2
⇒2V_1-V_2=10

I know it's bad, but I am finding this electrical element difficult.
:/ Worst case scenario if I put up what I have at least it shows I made the effort!
 
  • #11
amy1983 said:
I_3-I_4-I_5=0
⇒I_3=I_4+I_5
⇒(V_1-V_2)/(1 k)=(5+V_2)/(1 k)+V_2/(2 k)
⇒2(V_1-V_2 )=(10+2V_2 )+V_2
⇒2V_1-2V_2=10V_2+2V_2
You seem to be having difficulty expanding and then collecting terms. On the LHS you've got: 2*V1 - 2*V2. On the RHS you've got: 10 + 2*V2 + V2 = 10 + 3*V2. So:

2*V1 - 2*V2 = 10 + 3*V2

Move the 3*V2 from the RHS to the LHS by subtracting 3*V2 from both sides. Then proceed.
I know it's bad, but I am finding this electrical element difficult.
:/ Worst case scenario if I put up what I have at least it shows I made the effort!

I know it can be tricky, and much of circuit analysis involves a good deal of finicky algebra. But you are indeed showing good effort and insight for what you need to do to get the result. As they say, the devil is in the details :smile:
 

Related to 3 batteries, 5 resistors using KCL & KVL

1. What is KCL and KVL?

KCL (Kirchhoff's Current Law) states that the sum of currents entering a node in a circuit must equal the sum of currents leaving that node. KVL (Kirchhoff's Voltage Law) states that the sum of voltage drops in a closed loop must equal the sum of voltage sources in that loop.

2. How do KCL and KVL apply to a circuit with 3 batteries and 5 resistors?

KCL and KVL can be used to analyze the flow of currents and voltages in a circuit with multiple components, such as 3 batteries and 5 resistors. By applying these laws, we can determine the currents at different points in the circuit and the voltages across each component.

3. How can KCL and KVL help in solving circuit problems?

KCL and KVL provide a systematic approach to solving circuit problems by applying the principles of conservation of charge and energy. By using these laws, we can create equations that can be solved to determine the unknown currents and voltages in a circuit.

4. Are there any limitations to using KCL and KVL?

KCL and KVL are based on ideal conditions and may not always accurately reflect the behavior of real circuits. They also assume that the circuit is in steady-state, meaning that the currents and voltages are constant. In addition, KCL and KVL can only be applied to circuits that can be represented as a series or parallel combination of components.

5. How can I apply KCL and KVL in practical situations?

KCL and KVL are essential tools for circuit analysis and can be applied in various practical situations, such as designing and troubleshooting electronic circuits. By using these laws, we can determine the optimal values for resistors and other components in a circuit and identify any potential problems that may arise.

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