Kirchhoff's Voltage Law in a Battery

In summary, the problem involves two batteries with emfs of 9.0 V and 12.0 V, each with an internal resistance of 1.0 ohms, and three resistors with values of 25 ohms, 18 ohms, and 35 ohms. To find the direction and magnitude of the currents, Kirchhoff's laws must be applied. The easiest way to solve the problem is by using the principle of superposition, which involves solving the problem twice by deactivating each battery separately. Using this method, the currents can be found to be 0.68 A flowing right, 0.31 A flowing left, and 0.18 A flowing up. Alternatively, the problem
  • #1
jena
74
0
Hi,

My question:

The batteries have emfs of E1=9.0 V and E2= 12.0 V and the resistors have values of R1=25 ohms, R2=18 ohms, and R3=35 ohms.Assuming each battery has internal resistance r=1.0 ohms find the direction and magnitude of the currents.


____R1______
|.....|
E1......|
|_____R2______|
|.....|
E2......R3
|_____________|


For this problem could I use this equation to find the currents.

V(ab)=E-Ir and I= V/R

Is this correct :confused:

Thank You :smile:
 
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  • #2
jena said:
For this problem could I use this equation to find the currents.

V(ab)=E-Ir and I= V/R

Is this correct :confused:

Since you have not labeled nodes "a" and "b", it's not possible to say.
 
  • #3
Please disregard the ab nodes.

Thank You
 
  • #4
jena said:
For this problem could I use this equation to find the currents.

V(ab)=E-Ir and I= V/R

OK, even if we disregard the "ab", you still aren't going to solve this with a canned equation. You have to apply Kirchhoff's laws to the problem. I think that the easiest way to solve the problem is by superposition. That is, solve the problem once by deactivating E1 and solve it again by deactivating E2 (deactivated voltage sources are just short circuits). Then you can find the currents in each case and add the results together.
 
  • #5
So it would be

I=V/R

I(1)=E1/(R1+R2)

I(2)=E2/(R1+R3)

to help find the currents needed
 
  • #6
No, you have to apply Kirchhoff's laws. This requires some analysis beyond simple plug-and-chug.

As I was explaining, I think the easiest way to do this problem would be to look at the following two circuits:

____R1______
|.....|
E1......|
|_____R2______|
|.....|
|......R3
|_____________|

and

____R1______
|.....|
|.....|
|_____R2______|
|.....|
E2......R3
|_____________|

Find the current through each resistor for both circuits. Then you can add up the results for each circuit to get the current through each resistor when both sources are activated. This is called the principle of superposition, and it works because the element law for resistors (V=IR) is linear.
 
  • #7
Hi,

I have the currents:

I(1)=.68 A right
I(2)=.31 A left
I93)= .18 A up

what's next :confused:

Thank You :smile:
 
  • #8
Jena,

if 0.68 C/sec flows into the solder-spot on the right
(where R1 joins R2 and joins R3),
then 0.68 C/sec must flow OUT of that node.
(you have (0.31 - 0.18)[Amp] = 0.13 C/sec out.)

Why would I3 flow up? only if E2 is + at bottom.
But then I2 must be large.

You Did simplify with series and parallel R's first?
 
  • #9
Hi,

I tried it again and this time I set equations to find the currents using the loop rule.

Loop 1:

E1- I1(R1+r)-I2(R2), where is the r, is the internal resistance

____R1___>___
|......|
r.....|
E1.....V
|_____R2_<___|


Loop 2:
-E2+I2(R2)+I3(R3+r), again where r is the internal resistance

____R2___<___
^......|
|......|
E2.....^
|_r____R2_>___|

Is this correct :confused:

Thank You
 
  • #10
Hi,

I think I got it now, the work is below.

1. Set up loops

Loop 1: E1-(R1+r)(I1)-R2(I2)=0
9V-(25ohms+1ohms)(I1)-(18ohms)(I2)=0
9V-(26ohms)(I1)-(18ohms)(I2)=0

Loop 2: E2-(R3+r)(I3)-R2(I2)=0
12V-(35ohms+1ohms)(I1)-(18ohms)(I2)=0
12V-(36ohms)(I3)-(18ohms)(I2)=0

2. Substitution: Add Junctin equation in: I2= I1+I3

Loop 1: 9V-(26ohms)(I1)-(18ohms)(I2)=0
9V-(26ohms)(I1)-(18ohms)(I1+I3 )=0
9V-(44ohms)(I1)-(18ohms)(I3 )=0
-(44ohms)(I1)-(18ohms)(I3 )=-9V

Loop 2: 12V-(36ohms)(I3)-(18ohms)(I2)=0
12V-(36ohms)(I3)-(18ohms)(I1+I3 )=0
12V-(54ohms)(I3)-(18ohms)(I1 )=0
-(54hms)(I3)-(18ohms)(I1)=-12V

3. Add/Subtract Loop 1 and Loop 2. Solve for I3

Loop 1:18( -(46ohms)(I1)-(18ohms)(I3 )=-9V)
Loop 2: -44( -(54hms)(I3)-(18ohms)(I1)=-12V)

I3=(366 V)/(2052ohms)
I3=.178 A

4. Solve for I2, using loop 2

Loop 2:12V-(36ohms)(I3)-(18ohms)(I2)=0
12V-(36ohms)(.178 A)-(18ohms)(I2)=0
I2=.309 A

5. Sove for I1, using junction equation
Junction equation: I2=I1+I3
.309A= I1 +.178A
.309A -.178 A= I1
I1 =.131 A

Is this the correct way to do it :confused:

Thank You :smile:
 

1. What is Kirchhoff's Voltage Law in a Battery?

Kirchhoff's Voltage Law is a fundamental law in circuit analysis that states that the sum of all voltages around a closed loop in a circuit must equal zero. In the context of a battery, this means that the total voltage drop across all components in a circuit connected in series must equal the voltage of the battery.

2. How does Kirchhoff's Voltage Law apply to batteries?

In a battery-powered circuit, Kirchhoff's Voltage Law applies because the battery is the sole source of voltage in the circuit. The law ensures that all the voltage supplied by the battery is accounted for and used up by the components in the circuit.

3. Can Kirchhoff's Voltage Law be applied to circuits with multiple batteries?

Yes, Kirchhoff's Voltage Law can be applied to circuits with multiple batteries. In this case, each battery is treated as a separate voltage source, and the law is applied to each closed loop in the circuit.

4. What happens if Kirchhoff's Voltage Law is not satisfied in a battery-powered circuit?

If Kirchhoff's Voltage Law is not satisfied in a battery-powered circuit, it means that there is a discrepancy in the amount of voltage being supplied by the battery and the amount being used by the components in the circuit. This could be due to a faulty component or a mistake in the circuit design.

5. Can Kirchhoff's Voltage Law be violated?

No, Kirchhoff's Voltage Law cannot be violated. It is a fundamental law of circuit analysis that has been proven to hold true in all circuits. If the law appears to be violated, it is usually due to measurement errors or faulty components.

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