For The Circuit In Fig 3.51 Obtain V1 And V2

A Practical Look at Finding V1 and V2 in the Fig 3.51 Circuit

If you've ever cracked open an electric circuits textbook and landed on a figure labeled 3.51, you're probably staring at a network of resistors, maybe a dependent source, possibly two nodes you've been told to call V1 and V2, and a quiet little panic about where to begin. Honestly? That reaction is normal. The good news is that once you know which method to reach for, the problem usually unravels faster than it first looks.

Most textbook problems asking you to "obtain V1 and V2" for a circuit like the one in figure 3.So naturally, 51 are testing the same core skill: setting up and solving simultaneous equations using either nodal analysis or mesh analysis, depending on what the circuit gives you to work with. Because of that, the trick is knowing which one fits, writing the equations carefully, and not panicking when the algebra gets a little dense. Let's walk through it the way I'd explain it to a friend sitting next to me with the same problem in front of them.

What the Circuit in Fig 3.51 Actually Looks Like

The figure 3.51 circuit is a classic small-network problem. It typically shows a handful of resistors, one or two independent sources (a voltage source or current source), and often a dependent source whose value depends on one of the node voltages you're trying to find. The two unknowns, V1 and V2, are the voltages at two specific nodes relative to a reference (ground).

The reason this kind of problem shows up everywhere — Sadiku, Irwin, Nilsson, you name it — is that it hits the sweet spot of being simple enough to solve by hand but interesting enough to actually require real technique. You can't just eyeball it. You have to commit to a method.

Why People Get Stuck on This One

Here's what most students miss at first: the presence of a dependent source doesn't change the method*, only the order of operations*. You still write KCL or KVL equations at the same nodes or loops. The only extra step is that you substitute the controlling variable (often V1 or V2 themselves) after you've written the equations, not before.

The other common trap? Which means if you treat a current entering a node as positive in one equation and entering as positive in another, the matrix you build at the end will be wrong in a way that's hard to spot. Sign conventions. Pick a convention and stick with it across the entire problem.

And — real talk — a lot of people try to skip the algebra step. Because of that, they'll write one equation, glance at the circuit, and try to "feel" their way to the answer. Worth adding: that works for resistor-only problems sometimes. It almost never works once a dependent source is in the mix. Write the equations. Solve the equations. Then you can check your work.

How to Solve for V1 and V2 Step by Step

Step 1: Pick a Reference Node

Before you write a single equation, choose a node to call ground (0 V). And most of the time the figure already implies one — usually the bottom rail of the circuit, where the negative terminal of a source sits. If the figure is ambiguous, pick the node with the most branches connected to it. It usually makes the math cleaner.

Step 2: Label the Nodes

Mark V1 and V2 at the two nodes you care about. For the standard figure 3.If there are other non-reference nodes, label them too (V3, V4, whatever's needed). 31-style problem, you usually only need V1 and V2, but don't assume — count the nodes in the figure before committing.

Step 3: Choose Nodal or Mesh Analysis

Nodal analysis is almost always the better choice when you're asked for node voltages. And it directly gives you V1 and V2 as your unknowns, which means you don't have to back-solve from currents later. Mesh analysis still works, but you'll have to convert at the end.

So: nodal analysis unless the problem is clearly set up for mesh (rare in this kind of question).

Step 4: Apply KCL at Each Node

At node V1, sum the currents leaving the node through each connected branch and set them equal to zero (or equal to any current source flowing in). At node V2, do the same.

Each branch's current is expressed in terms of the node voltages using Ohm's law. If it connects V1 to V2, the current from V1 toward V2 is (V1 − V2)/R. Now, if a resistor R connects node V1 to ground, the current through it is V1/R. Take your time here — this is where most errors creep in.

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For a typical figure 3.51 setup, your two KCL equations will look something like:

At node V1: a·V1 + b·V2 = c

At node V2: d·V1 + e·V2 = f

Where a, b, c, d, e, and f are combinations of resistor values and source values. The exact numbers depend on the resistors in your specific figure.

Step 5: Handle the Dependent Source

If the circuit has a dependent source (say, a current source whose value is k·V1, or a voltage source controlled by some other quantity), treat it like any other source when you write KCL — except don't substitute its value yet. Write the KCL equation with the dependent source's symbol in it. Then, after you've got your system of equations, substitute the controlling variable.

Take this: if a current source equals 2·V1, and it flows into node V2, your KCL at node V2 will include a term like +2·V1 on the right-hand side.

Step 6: Solve the System

You have two linear equations in two unknowns. You can solve them by substitution, elimination, or matrix methods. For a 2×2 system, Cramer's rule is quick and clean:

V1 = (c·e − b·f) / (a·e − b·d)

V2 = (a·f − c·d) / (a·e − b·d)

Just watch out for division by zero — that would mean your equations are linearly dependent, which usually signals an error in how you set them up.

Common Mistakes People Make

Mixing up resistor positions. A 2 kΩ resistor between V1 and V2 is not the same as two 2 kΩ resistors in series from V1 to V2 through an intermediate node. Count the actual branches in the figure.

Forgetting the dependent source's sign. If the arrow on a dependent current source points into* a node, it contributes positively to the current entering that node. If it points out, it contributes negatively. Sounds obvious, but it's the single most common error in these problems.

Substituting too early. If a dependent source is controlled by V1, leave it symbolic until you've set up the full system. Substituting immediately can lock you into the wrong sign or value.

Losing track of units. V1 and V2 are in volts. Currents from current sources are in amps. Resistor values need to be in consistent units (usually kΩ paired with mA, or Ω paired with A) or your equation will be off by a factor of a thousand. This is the kind of mistake that doesn't show up until the very end, when the answer is "weird."

Solving the wrong pair of equations. If the circuit has more than two non-reference nodes, make sure you're solving for V1 and V2 specifically — not V1 and V3, or V2 and V3.

What Actually Helps in Practice

A few things that aren't in textbooks but make these problems much less painful:

• Redraw the circuit. Especially if the figure is cramped. Spread the nodes out, label everything clearly, and mark the assumed polarity of V1 and V2.
• Write the KCL equations in words first. "Sum of currents leaving V1 equals zero" sounds redundant, but it forces you to think about each branch individually instead of pattern-matching from memory.
• Check your answer with KCL at the end. Plug your V1 and V2 back into the original KCL equations. If both equations balance, you're almost certainly right. If one is off by a small amount, you've got a sign error somewhere.
• If the answer involves a dependent source, sanity-check the sign. A voltage that's supposed to depend on V1 should change sign in a way that makes physical sense given the circuit's polarity.