Convert the circuit shown in fig. into a single voltage source in series with resistance.
Source transformation is a fundamental and powerful technique in electrical circuit analysis. It allows you to simplify a complex circuit by replacing a voltage source in series with a resistor with an equivalent current source in parallel with the same resistor, and vice-versa. This method, rooted in Thevenin's and Norton's theorems, makes solving for currents and voltages in a network significantly easier.
In this guide, we will walk through a complete example of simplifying a circuit into a single equivalent voltage source and series resistor.
Question: Convert the circuit shown in the figure into a single voltage source in series with a resistor.
Original Circuit Diagram:
The initial circuit contains:
A 50V voltage source in series with a 5Ω resistor on the left branch.
A 10V voltage source in series with a 3Ω resistor on the right branch.
* A 10A independent current source and a 2Ω resistor in the central bridge structure.
To solve this, we will convert all voltage sources into current sources, combine the parallel components, and then convert the final simplified circuit back into a voltage source.
First, we'll transform the leftmost branch. A voltage source (V) in series with a resistor (R) is equivalent to a current source (I) in parallel with the same resistor (R).
The 5Ω resistor is now placed in parallel with this new 10A current source. The direction of the current arrow points towards the positive terminal of the original voltage source (upwards).
Next, we apply the same transformation to the rightmost branch of the circuit.
The 3Ω resistor is now in parallel with the 10/3 A current source. The arrow also points upwards, toward the original positive terminal.
After the transformations, our circuit consists of only current sources and resistors, all connected between the same two nodes. This means all three resistors (5Ω, 2Ω, and 3Ω) are in parallel. We can combine them into a single equivalent resistor (Req).
Just like the resistors, all three current sources are now in parallel. Since their current arrows all point in the same direction (upwards), we can simply add their values to find the total equivalent current (I_total).
The final step is to convert this simplified Norton equivalent circuit back into a Thevenin equivalent circuit (a voltage source in series with a resistor), as requested by the problem.
The original circuit can be simplified into a single equivalent circuit consisting of a 22.58 V voltage source in series with a 30/31 Ω (or approximately 0.97 Ω) resistor.
Final Circuit Diagram: