Find the current in branch AB of the circuit shown in fig. using Source transformation
This article provides a detailed solution for finding the current in branch AB of the given electrical circuit. The method used is Source Transformation, a powerful technique in circuit analysis for simplifying complex circuits.
Question: Find the current flowing through branch AB of the circuit shown in the figure using the source transformation method.
Original Circuit Diagram:
The circuit consists of:
A 6V voltage source in series with a 15Ω resistor on the left.
A 6V voltage source in series with an 8Ω resistor on the right.
A 5Ω resistor and an 8Ω resistor in the central part of the circuit.
A 10Ω resistor connecting nodes A and B (this is branch AB).
The goal is to simplify the circuit into a single loop to easily calculate the current I
flowing through the 10Ω resistor in branch AB.
Source transformation allows us to convert a voltage source in series with a resistor into an equivalent current source in parallel with the same resistor. The formula is I = V / R.
Left Side Transformation:
The 6V source and the 15Ω series resistor are converted to a current source.
I_left = V / R = 6V / 15Ω = 0.4A
This results in a 0.4A current source (with the arrow pointing up) in parallel with the 15Ω resistor.
Right Side Transformation:
The 6V source and the 8Ω series resistor are converted to a current source.
I_right = V / R = 6V / 8Ω = 0.75A
This results in a 0.75A current source (with the arrow pointing up) in parallel with the 8Ω resistor.
The circuit now looks like this:
Now, we can simplify the circuit by combining the resistors that are in parallel.
Left Side Resistors:
The 15Ω resistor and the 5Ω resistor are in parallel.
R_left = 15Ω || 5Ω = (15 × 5) / (15 + 5) = 75 / 20 = 3.75Ω
Right Side Resistors:
The two 8Ω resistors are in parallel.
R_right = 8Ω || 8Ω = (8 × 8) / (8 + 8) = 64 / 16 = 4Ω
The simplified circuit becomes:
To create a final, single-loop circuit, we transform the current sources back into voltage sources. The formula is V = I × R.
Left Side Transformation:
The 0.4A current source and the 3.75Ω parallel resistor are converted back to a voltage source.
V_left = I × R = 0.4A × 3.75Ω = 1.5V
This results in a 1.5V voltage source in series with the 3.75Ω resistor.
Right Side Transformation:
The 0.75A current source and the 4Ω parallel resistor are converted back to a voltage source.
V_right = I × R = 0.75A × 4Ω = 3V
This results in a 3V voltage source in series with the 4Ω resistor.
This gives us the final single-loop circuit:
We can now find the current I
in branch AB by applying KVL to the single loop. Let's assume the current I
flows in a clockwise direction (from A to B).
Applying KVL by traversing the loop clockwise:
-1.5V + (3.75Ω × I) + (10Ω × I) + (4Ω × I) + 3V = 0
Now, we solve the KVL equation for I
.
Combine the terms with I
:
(3.75 + 10 + 4) × I + (-1.5 + 3) = 0
Simplify the equation:
17.75 × I + 1.5 = 0
Isolate I
:
17.75 × I = -1.5
Solve for I
:
I = -1.5 / 17.75
I ≈ -0.0845 A
To express the answer in milliamps (mA), multiply by 1000:
I = -0.0845 A × 1000 = -84.5 mA
The current flowing in branch AB is:
I = -84.5 mA
The negative sign indicates that the actual direction of the current is opposite to our assumed clockwise direction. Therefore, the current of 84.5 mA flows from node B to node A.