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rewrite the same as given below : Here's the neatly rewritten version of your handwritten solution using the **Mesh Analysis Method**: --- ### **Mesh Analysis Method** --- #### **For Loop Current $i_1$** Using mesh analysis, we get: $$ (1 - j2)i_1 - i_2 = 12\angle 0^\circ \tag{1} $$ --- #### **From the Circuit:** $$ v_{in} = 14\angle 0^\circ = j5 \cdot x_{i_3} + j2 \cdot x_{i_1} $$ And since: $$ i_g = i_2 = 2 \cdot v_{in} = 2 \left[14\angle 0^\circ + j5 \cdot x_{i_3} + j2 \cdot x_{i_1} \right] $$ $$ = 28\angle 0^\circ + j10 \cdot x_{i_3} + j4 \cdot x_{i_1} \tag{2} $$ --- #### **For Loop Currents $i_2$ and $i_3$:** Applying **supermesh analysis**, we get: $$ j3 \cdot x_{i_2} + \left[ (1 \angle 0^\circ)(i_2 - i_1) \right] - j5 \cdot x_{i_3} + 4(i_3 - i_4) = 0 $$ Simplifying: $$ - i_1 + (1 + j3)i_2 + (4 - j5)i_3 - 4i_4 = 0 \tag{3} $$ --- Here is the neatly rewritten version of your solution (page 2): --- ### **From the circuit,** $$ I_x = i_4 - i_5 = i_4 + 2\angle 0^\circ \quad \text{(since } i_5 = -2\angle 0^\circ \text{ from circuit)} $$ --- ### **For Loop Current $i_4$:** Using mesh analysis, we get: $$ j6 \cdot i_4 + 4(i_4 - i_3) + 3(i_4 + 2\angle 0^\circ) = 0 $$ Expanding: $$ -4i_3 + (7 + j6)i_4 = -6\angle 0^\circ \tag{4} $$ --- ### **From Equations (1), (2), (3), and (4):** Solving the system, we get: $$ i_1 = [2.27 + j\,4.935]\, \text{A} $$ $$ i_2 = [0.1502 + j\,0.338]\, \text{A} $$ $$ i_3 = [-0.8566 + j\,0.926]\, \text{A} $$ $$ i_4 = [-0.514 + j\,0.97]\, \text{A} $$ --- ### **Compute $I_x$:** $$ I_x = i_4 + 2\angle 0^\circ = [1.486 + j\,0.97]\, \text{A} $$ Convert to polar form: $$ I_x = 1.774 \angle 33.13^\circ \, \text{A} $$ --- ### **Compute $V_x$:** $$ V_x = 0.562 \angle 152.79^\circ \, \text{Volts} $$ ---

Question:

rewrite the same as given below : Here's the neatly rewritten version of your handwritten solution using the **Mesh Analysis Method**: --- ### **Mesh Analysis Method** --- #### **For Loop Current $i_1$** Using mesh analysis, we get: $$ (1 - j2)i_1 - i_2 = 12\angle 0^\circ \tag{1} $$ --- #### **From the Circuit:** $$ v_{in} = 14\angle 0^\circ = j5 \cdot x_{i_3} + j2 \cdot x_{i_1} $$ And since: $$ i_g = i_2 = 2 \cdot v_{in} = 2 \left[14\angle 0^\circ + j5 \cdot x_{i_3} + j2 \cdot x_{i_1} \right] $$ $$ = 28\angle 0^\circ + j10 \cdot x_{i_3} + j4 \cdot x_{i_1} \tag{2} $$ --- #### **For Loop Currents $i_2$ and $i_3$:** Applying **supermesh analysis**, we get: $$ j3 \cdot x_{i_2} + \left[ (1 \angle 0^\circ)(i_2 - i_1) \right] - j5 \cdot x_{i_3} + 4(i_3 - i_4) = 0 $$ Simplifying: $$ - i_1 + (1 + j3)i_2 + (4 - j5)i_3 - 4i_4 = 0 \tag{3} $$ --- Here is the neatly rewritten version of your solution (page 2): --- ### **From the circuit,** $$ I_x = i_4 - i_5 = i_4 + 2\angle 0^\circ \quad \text{(since } i_5 = -2\angle 0^\circ \text{ from circuit)} $$ --- ### **For Loop Current $i_4$:** Using mesh analysis, we get: $$ j6 \cdot i_4 + 4(i_4 - i_3) + 3(i_4 + 2\angle 0^\circ) = 0 $$ Expanding: $$ -4i_3 + (7 + j6)i_4 = -6\angle 0^\circ \tag{4} $$ --- ### **From Equations (1), (2), (3), and (4):** Solving the system, we get: $$ i_1 = [2.27 + j\,4.935]\, \text{A} $$ $$ i_2 = [0.1502 + j\,0.338]\, \text{A} $$ $$ i_3 = [-0.8566 + j\,0.926]\, \text{A} $$ $$ i_4 = [-0.514 + j\,0.97]\, \text{A} $$ --- ### **Compute $I_x$:** $$ I_x = i_4 + 2\angle 0^\circ = [1.486 + j\,0.97]\, \text{A} $$ Convert to polar form: $$ I_x = 1.774 \angle 33.13^\circ \, \text{A} $$ --- ### **Compute $V_x$:** $$ V_x = 0.562 \angle 152.79^\circ \, \text{Volts} $$ ---

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Asked by: mohit
Created at: 2025-08-04 00:22:24

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Certainly! Here’s your solution, **rewritten in a clear, organized format using the Mesh Analysis Method**: --- ## **Mesh Analysis Method** --- ### **1. For Loop Current $i_1$** Applying mesh analysis: $$ (1 - j2)i_1 - i_2 = 12\angle 0^\circ \tag{1} $$ --- ### **2. From the Circuit** The input voltage is given by: $$ v_{in} = 14\angle 0^\circ = j5 \cdot i_3 + j2 \cdot i_1 $$ Given that: $$ i_g = i_2 = 2 \cdot v_{in} = 2 \left[14\angle 0^\circ + j5i_3 + j2i_1 \right] $$ $$ = 28\angle 0^\circ + j10i_3 + j4i_1 \tag{2} $$ --- ### **3. For Loop Currents $i_2$ and $i_3$ (Supermesh)** Applying supermesh analysis: $$ j3\,i_2 + \left[ 1\angle 0^\circ (i_2 - i_1) \right] - j5\,i_3 + 4(i_3 - i_4) = 0 $$ Simplifying: $$ - i_1 + (1 + j3)i_2 + (4 - j5)i_3 - 4i_4 = 0 \tag{3} $$ --- ### **4. For Loop Current $i_4$** From the circuit: $$ I_x = i_4 - i_5 = i_4 + 2\angle 0^\circ \quad \text{(since } i_5 = -2\angle 0^\circ \text{)} $$ Applying mesh analysis: $$ j6\,i_4 + 4(i_4 - i_3) + 3(i_4 + 2\angle 0^\circ) = 0 $$ Expanding: $$ -4i_3 + (7 + j6)i_4 = -6\angle 0^\circ \tag{4} $$ --- ### **5. Solving the System (Equations 1–4)** By solving the above equations, we obtain: $$ i_1 = 2.27 + j\,4.935 \ \text{A} $$ $$ i_2 = 0.1502 + j\,0.338 \ \text{A} $$ $$ i_3 = -0.8566 + j\,0.926 \ \text{A} $$ $$ i_4 = -0.514 + j\,0.97 \ \text{A} $$ --- ### **6. Finding $I_x$** $$ I_x = i_4 + 2\angle 0^\circ = 1.486 + j\,0.97 \ \text{A} $$ **In polar form:** $$ I_x = 1.774 \angle 33.13^\circ \ \text{A} $$ --- ### **7. Finding $V_x$** $$ V_x = 0.562 \angle 152.79^\circ \ \text{Volts} $$ --- **Final Answers:** - $\boxed{I_x = 1.774 \angle 33.13^\circ \ \text{A}}$ - $\boxed{V_x = 0.562 \angle 152.79^\circ \ \text{V}}$ ---

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