1. 2. 3. 4. 5. In Rn Eth Rth VL(Min) VL(Max) IL(Min) IL(Max) R₁ max pwr

Introductory Circuit Analysis (13th Edition)
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ISBN:9780133923605
Author:Robert L. Boylestad
Publisher:Robert L. Boylestad
Chapter1: Introduction
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I have included the circuit in question as well as the questions/data table, thanks.

### Educational Circuit Analysis Worksheet

This worksheet is designed to help students analyze and calculate key parameters in electrical circuits. Below are the components and variables typically involved in analyzing circuit performance:

1. **Thevenin's Equivalent Parameters**
   - **Eth**: Thevenin's Equivalent Voltage
   - **Rth**: Thevenin's Equivalent Resistance

2. **Current Analysis**
   - **In**: Current through circuit prior to load
   - **Rn**: Resistance affecting current calculation

3. **Load Voltage Evaluation**
   - **V<sub>L(Min)</sub>**: Minimum Load Voltage
   - **V<sub>L(Max)</sub>**: Maximum Load Voltage

4. **Load Current Evaluation**
   - **I<sub>L(Min)</sub>**: Minimum Load Current
   - **I<sub>L(Max)</sub>**: Maximum Load Current

5. **Load Resistance for Maximum Power Transfer**
   - **R<sub>L max pwr</sub>**: Load Resistance for Maximum Power Transfer

These parameters aid in determining the efficiency and performance of an electrical circuit, particularly when converting to the Thevenin equivalent model. By calculating and analyzing these values, students can gain a thorough understanding of how different elements within a circuit interact.

Note: Blank spaces provided next to each parameter allow students to input or calculate the necessary values during analysis exercises.
Transcribed Image Text:### Educational Circuit Analysis Worksheet This worksheet is designed to help students analyze and calculate key parameters in electrical circuits. Below are the components and variables typically involved in analyzing circuit performance: 1. **Thevenin's Equivalent Parameters** - **Eth**: Thevenin's Equivalent Voltage - **Rth**: Thevenin's Equivalent Resistance 2. **Current Analysis** - **In**: Current through circuit prior to load - **Rn**: Resistance affecting current calculation 3. **Load Voltage Evaluation** - **V<sub>L(Min)</sub>**: Minimum Load Voltage - **V<sub>L(Max)</sub>**: Maximum Load Voltage 4. **Load Current Evaluation** - **I<sub>L(Min)</sub>**: Minimum Load Current - **I<sub>L(Max)</sub>**: Maximum Load Current 5. **Load Resistance for Maximum Power Transfer** - **R<sub>L max pwr</sub>**: Load Resistance for Maximum Power Transfer These parameters aid in determining the efficiency and performance of an electrical circuit, particularly when converting to the Thevenin equivalent model. By calculating and analyzing these values, students can gain a thorough understanding of how different elements within a circuit interact. Note: Blank spaces provided next to each parameter allow students to input or calculate the necessary values during analysis exercises.
**Figure 7-1 Description:**

The diagram shows an electrical network with a voltage source \(E = 15 \, \text{V}\) and three resistors arranged as follows:

- \(R_1 = 4.7 \, \text{k}\Omega\) in series with \(R_2 = 3.3 \, \text{k}\Omega\).
- \(R_3 = 680 \, \Omega\) in parallel with the series combination of \(R_1\) and \(R_2\).
- A pair of output terminals labeled \(a\) and \(b\) are connected to a variable load resistor \(R_L\) which can vary from \(0\) to \(10 \, \text{k}\Omega\). The output voltage across these terminals is labeled \(V_L\).

**Text Details:**

**Thévenin’s Theorem:**

Any linear bilateral network may be reduced to a simplified two-terminal network consisting of a single voltage source, \(E_{\text{Th}}\), in series with a single resistor, \(R_{\text{Th}}\). Once the original network is simplified, any load connected to the output terminals will behave exactly as if the load were connected in series with \(E_{\text{Th}}\) and \(R_{\text{Th}}\).

**Norton’s Theorem:**

Any linear bilateral network may be reduced to a simplified two-terminal network consisting of a single current source, \(I_N\), in parallel with a single resistor, \(R_N\). A Thévenin equivalent circuit is easily converted into a Norton equivalent by performing a source conversion as follows:

\[
R_N = R_{\text{Th}} \quad (7-1)
\]

\[
I_N = \frac{E_{\text{Th}}}{R_{\text{Th}}} \quad (7-2)
\]

When a load is connected across the output terminals, the circuit will behave exactly as if the load were connected in parallel with \(I_N\) and \(R_N\).

**Maximum Power Transfer Theorem:**

Maximum power will be delivered to the load resistance when the load resistance is equal to the Thévenin (or Norton) resistance.
Transcribed Image Text:**Figure 7-1 Description:** The diagram shows an electrical network with a voltage source \(E = 15 \, \text{V}\) and three resistors arranged as follows: - \(R_1 = 4.7 \, \text{k}\Omega\) in series with \(R_2 = 3.3 \, \text{k}\Omega\). - \(R_3 = 680 \, \Omega\) in parallel with the series combination of \(R_1\) and \(R_2\). - A pair of output terminals labeled \(a\) and \(b\) are connected to a variable load resistor \(R_L\) which can vary from \(0\) to \(10 \, \text{k}\Omega\). The output voltage across these terminals is labeled \(V_L\). **Text Details:** **Thévenin’s Theorem:** Any linear bilateral network may be reduced to a simplified two-terminal network consisting of a single voltage source, \(E_{\text{Th}}\), in series with a single resistor, \(R_{\text{Th}}\). Once the original network is simplified, any load connected to the output terminals will behave exactly as if the load were connected in series with \(E_{\text{Th}}\) and \(R_{\text{Th}}\). **Norton’s Theorem:** Any linear bilateral network may be reduced to a simplified two-terminal network consisting of a single current source, \(I_N\), in parallel with a single resistor, \(R_N\). A Thévenin equivalent circuit is easily converted into a Norton equivalent by performing a source conversion as follows: \[ R_N = R_{\text{Th}} \quad (7-1) \] \[ I_N = \frac{E_{\text{Th}}}{R_{\text{Th}}} \quad (7-2) \] When a load is connected across the output terminals, the circuit will behave exactly as if the load were connected in parallel with \(I_N\) and \(R_N\). **Maximum Power Transfer Theorem:** Maximum power will be delivered to the load resistance when the load resistance is equal to the Thévenin (or Norton) resistance.
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