These are the two cases in solving the circuit problem:
1st Case: When the voltage source is connected to non-reference node and a reference node or ground.
2nd Case: The Supernode. It is when the voltage source is not connected to the ground or reference node.
Let us analyze such cases by these examples:
#1: Consider this circuit.
Here are the steps in solving a circuit:
1. Analyze the problem.
2. Assign nodes. Assume that I am going to assign V1 as my first node, and V2 as my second node.
3. Since the 12 volts source is given and is connected to the non-reference and a reference node, then V1 is 12V. We have now the exact value of the first node.
4. Solve V2 by adding the quantities of the following:
Since V1 = 12 /_0V; then
V2(1/3 - 1/j1 + 1/j2) - 12V/3 = 0
0.33 + j0.5V2 - 6 = 0
0.33 + j0.5V2 = 6
V2 = 5.538 - j8.307 or
V2 = 9.98 /_ -146.309 Volts
And now we get Io value:
Io = V/R
= 9.98/_ -146.309 / j2
Io = 4.99/_ -146.309 Amps
Io = V/R
= 9.98/_ -146.309 / j2
Io = 4.99/_ -146.309 Amps
#2: Consider this Circuit:
Solve for V1 and V2
1. Analyze the problem.
2. Look at the figure again. As what we saw, the 12 volts source is not connected to the reference node. Then I conclude that it is a supernode.
3. Assign nodes again. Assume that I am going to assign V1 as my first node, and V2 as my second node.
4. Join the two nodes as a supernode.
5. Remove the voltage source by changing it in a short circuit. (Take note as well: that if the current source is given and has to be removed, change it in an open circuit.)
6. In getting the value of a supernode, get the equation value by using Kirchoff's Current Law(KCL):
@KCL:
I1 + I2 + I3 = 0
- I1 = V1/R1 = V1/3
- I2 = V2/-j1
- I3 = V2/j2
V1/3 + V2/-j1 + V2/j2 = 0
@KVL:
V1+12/_0 - V2 = 0
V1-V2 = -12/_0
V1 = V2 - 12/_0
Now get the values:
V2 - 12/3 + (V2/-j1) + V2/j2 = 0
V2/3 - 6 +(V2/-j1)+V2/j2 = 0
V2(1/3 + (1/-j1) + 1/j2) = 6
0.33V2 + j0.5 = 6
V2 = 9.98/_ -56.309 V
V1 = 9.98/_ -56.309 - 12
V1 = 10.52/_ -127.89 V
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