Give step-by-step solution with explanation and final answer:A 0 el 8 - 1 Za A 9p : HE Z.n A (Ph Bari 4: can Sil | a) Using Source transformation and Nodal method, find V1, Va and Vs b) Find Power at the 4Q resistor.
Question:
Give step-by-step solution with explanation and final answer:
A 0 el 8 - 1
Za A 9p
: HE Z.n A (Ph
Bari 4: can Sil |
a) Using Source transformation and Nodal
method, find V1, Va and Vs
b) Find Power at the 4Q resistor.
This is AI generated Response.
Asked by: M Raju
Created at: 2025-09-17 22:47:34
Asked by: M Raju
Created at: 2025-09-17 22:47:34
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Let's solve the circuit step-by-step as requested:
---
## Step 1: **Redraw the Circuit with Node Labels**
Let's denote:
- \( V_1 \): Voltage at the node between \( 1\Omega \), \( 4\Omega \), and \( 2\Omega \) resistors (left).
- \( V_2 \): Voltage at the node between \( 2\Omega \), \( 2\Omega \), and \( 2\Omega \) resistors (middle).
- \( V_3 \): Voltage at the node between \( 2\Omega \), \( 2\Omega \), and \( 2A \) source (right).
---
### **Node Assignment**
- The leftmost node (ground reference) is at 0V.
- The rightmost node (bottom, after \( 2A \) current source) is taken as reference (0V).
---
## Step 2: **Source Transformation**
The 40V voltage source in series with \( 1\Omega \) can be transformed into a current source:
\[
I = \frac{40V}{1\Omega} = 40A
\]
So, this becomes a \( 40A \) current source in parallel with \( 1\Omega \).
However, for nodal analysis, we can keep it as is for simplicity.
---
## Step 3: **Nodal Analysis**
Let's assign the nodes as shown in the image:
- Node 1: \( V_1 \)
- Node 2: \( V_2 \)
- Node 3: \( V_3 \) (rightmost node before the current source)
### **Write KCL at Each Node**
#### **Node 1 (\( V_1 \)):**
Connected to:
- \( 1\Omega \) to ground (left)
- \( 4\Omega \) to \( V_2 \)
- \( 2\Omega \) to top (which connects to \( V_2 \))
Current leaving node:
\[
\frac{V_1}{1} + \frac{V_1 - V_2}{4} + \frac{V_1 - V_2}{2} = 0
\]
Simplify:
\[
\frac{V_1}{1} + \frac{V_1 - V_2}{4} + \frac{V_1 - V_2}{2} = 0
\]
\[
V_1 + \frac{V_1 - V_2}{4} + \frac{V_1 - V_2}{2} = 0
\]
\[
V_1 + \frac{V_1 - V_2 + 2(V_1 - V_2)}{4} = 0
\]
\[
V_1 + \frac{3(V_1 - V_2)}{4} = 0
\]
\[
4V_1 + 3(V_1 - V_2) = 0
\]
\[
4V_1 + 3V_1 - 3V_2 = 0
\]
\[
7V_1 - 3V_2 = 0 \implies 7V_1 = 3V_2 \implies V_1 = \frac{3}{7}V_2
\]
#### **Node 2 (\( V_2 \)):**
Connected to:
- \( 4\Omega \) to \( V_1 \)
- \( 2\Omega \) to \( V_1 \) (top)
- \( 2\Omega \) to \( V_3 \)
- \( 2\Omega \) to top right node
- \( 2A \) current source (leaving node)
Write KCL:
\[
\frac{V_2 - V_1}{4} + \frac{V_2 - V_1}{2} + \frac{V_2 - V_3}{2} + 2 = 0
\]
Simplify:
\[
\frac{V_2 - V_1}{4} + \frac{V_2 - V_1}{2} + \frac{V_2 - V_3}{2} = -2
\]
\[
\frac{V_2 - V_1 + 2(V_2 - V_1) + 2(V_2 - V_3)}{4} = -2
\]
\[
\frac{3(V_2 - V_1) + 2(V_2 - V_3)}{4} = -2
\]
\[
3(V_2 - V_1) + 2(V_2 - V_3) = -8
\]
\[
3V_2 - 3V_1 + 2V_2 - 2V_3 = -8
\]
\[
(3V_2 + 2V_2) - 3V_1 - 2V_3 = -8
\]
\[
5V_2 - 3V_1 - 2V_3 = -8
\]
#### **Node 3 (\( V_3 \)):**
Connected to:
- \( 2\Omega \) to \( V_2 \)
- \( 2\Omega \) to ground
KCL:
\[
\frac{V_3 - V_2}{2} + \frac{V_3}{2} = 0
\]
\[
\frac{V_3 - V_2 + V_3}{2} = 0
\]
\[
V_3 - V_2 + V_3 = 0
\]
\[
2V_3 - V_2 = 0
\]
\[
2V_3 = V_2 \implies V_3 = \frac{V_2}{2}
\]
---
### **Now substitute relationships:**
Recall:
- \( V_1 = \frac{3}{7}V_2 \)
- \( V_3 = \frac{V_2}{2} \)
Plug into equation for Node 2:
\[
5V_2 - 3V_1 - 2V_3 = -8
\]
\[
5V_2 - 3\left(\frac{3}{7}V_2\right) - 2\left(\frac{V_2}{2}\right) = -8
\]
\[
5V_2 - \frac{9}{7}V_2 - V_2 = -8
\]
\[
5V_2 - V_2 - \frac{9}{7}V_2 = -8
\]
\[
4V_2 - \frac{9}{7}V_2 = -8
\]
\[
\left(4 - \frac{9}{7}\right)V_2 = -8
\]
\[
\left(\frac{28}{7} - \frac{9}{7}\right)V_2 = -8
\]
\[
\frac{19}{7}V_2 = -8
\]
\[
V_2 = -8 \cdot \frac{7}{19}
\]
\[
V_2 = -\frac{56}{19} \approx -2.95V
\]
---
### **Now calculate \( V_1 \) and \( V_3 \):**
\[
V_1 = \frac{3}{7}V_2 = \frac{3}{7} \times -2.95 \approx -1.27\text{ V}
\]
\[
V_3 = \frac{V_2}{2} = \frac{-2.95}{2} = -1.475\text{ V}
\]
---
## **Final Answers for (a):**
\[
\boxed{
V_1 \approx -1.27\text{ V} \V_2 \approx -2.95\text{ V} \\
V_3 \approx -1.48\text{ V}
}
\]
---
## Step 4: **Find Power at the \( 4\Omega \) Resistor (b):**
The current through the \( 4\Omega \) resistor:
\[
I_{4\Omega} = \frac{V_1 - V_2}{4}
\]
Plug in the values:
\[
I_{4\Omega} = \frac{-1.27 - (-2.95)}{4} = \frac{1.68}{4} = 0.42\text{ A}
\]
Power dissipated:
\[
P = I^2 R = (0.42)^2 \times 4 \approx 0.1764 \times 4 = 0.71\text{ W}
\]
---
## **Final Answer for (b):**
\[
\boxed{
\text{Power at the } 4\Omega \text{ resistor} = 0.71\text{ W}
}
\]
---
### **Summary Table**
| | Value |
|---|------------|
| \(V_1\) | -1.27 V |
| \(V_2\) | -2.95 V |
| \(V_3\) | -1.48 V |
| \(P_{4\Omega}\) | 0.71 W |
---
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