Construct the frequency-domain equivalent circuit.

Introductory Circuit Analysis (13th Edition)
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ISBN:9780133923605
Author:Robert L. Boylestad
Publisher:Robert L. Boylestad
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Construct the frequency-domain equivalent circuit.
## 3. Frequency-Domain

The sinusoidal voltage sources in the circuit shown in Figure 3 are:

- \( v_a(t) = V_a \cos(11t + \pi/13); \) and
- \( v_b(t) = V_b \sin(11t + \pi/17). \)

Construct the frequency-domain equivalent circuit.

### Description of Figure 3
Figure 3 depicts an electric circuit operating in the sinusoidal steady state, represented in the time-domain. The circuit consists of the following components:

- A sinusoidal voltage source \( v_a(t) \) on the left.
- A resistor with a resistance of 2 Ω connected in series at the top.
- In parallel with the resistor, there is a branch containing:
  - A capacitor labeled as 3 F (farads).
  - A resistor with a resistance of 5 Ω.
- A sinusoidal voltage source \( v_b(t) \) on the right.
- An inductor labeled as 7 H (henrys) connected in series at the right side.

This circuit is used to illustrate frequency-domain analysis by transforming time-domain sinusoidal sources into their equivalent phasors.
Transcribed Image Text:## 3. Frequency-Domain The sinusoidal voltage sources in the circuit shown in Figure 3 are: - \( v_a(t) = V_a \cos(11t + \pi/13); \) and - \( v_b(t) = V_b \sin(11t + \pi/17). \) Construct the frequency-domain equivalent circuit. ### Description of Figure 3 Figure 3 depicts an electric circuit operating in the sinusoidal steady state, represented in the time-domain. The circuit consists of the following components: - A sinusoidal voltage source \( v_a(t) \) on the left. - A resistor with a resistance of 2 Ω connected in series at the top. - In parallel with the resistor, there is a branch containing: - A capacitor labeled as 3 F (farads). - A resistor with a resistance of 5 Ω. - A sinusoidal voltage source \( v_b(t) \) on the right. - An inductor labeled as 7 H (henrys) connected in series at the right side. This circuit is used to illustrate frequency-domain analysis by transforming time-domain sinusoidal sources into their equivalent phasors.
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