Give step-by-step solution with explanation and final answer: The voltage at the terminals of a load is 2 5 0 V ( rms ) . The load is absorbing an average power of 4 0 KW and delivering a magnetizing reactive power of 3 0 kVAR. Find load resistance and reactance.
Question:
Give step-by-step solution with explanation and final answer: The voltage at the terminals of a load is 2 5 0 V ( rms ) . The load is absorbing an average power of 4 0 KW and delivering a magnetizing reactive power of 3 0 kVAR. Find load resistance and reactance.
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Asked by: aj
Created at: 2025-05-25 10:26:30
Asked by: aj
Created at: 2025-05-25 10:26:30
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Let's break down and solve the problem step by step:
**Given:**
- Terminal voltage, \( V_{rms} = 250 \) V
- Load absorbs average (real) power, \( P = 40 \) kW = \( 40,000 \) W
- Load delivers magnetizing reactive power, \( Q = 30 \) kVAR = \( 30,000 \) VAR
We are asked to **find the load resistance (\( R \)) and reactance (\( X \))**.
---
## **Step 1: Find Apparent Power and Load Impedance**
The complex power \( S \) is:
\[
S = P + jQ
\]
\[
|S| = \sqrt{P^2 + Q^2}
\]
Plug in the values:
\[
|S| = \sqrt{(40,000)^2 + (30,000)^2}
\]
\[
= \sqrt{1,600,000,000 + 900,000,000}
\]
\[
= \sqrt{2,500,000,000}
\]
\[
= 50,000 \text{ VA}
\]
---
## **Step 2: Find the Load Current**
\[
|S| = V_{rms} \cdot I_{rms}
\]
So,
\[
I_{rms} = \frac{|S|}{V_{rms}}
\]
\[
I_{rms} = \frac{50,000}{250} = 200 \text{ A}
\]
---
## **Step 3: Find Load Impedance**
The impedance \( Z \) is:
\[
Z = \frac{V_{rms}}{I_{rms}}
\]
\[
Z = \frac{250}{200} = 1.25 \ \Omega
\]
---
## **Step 4: Find Power Factor Angle**
The power factor angle \( \theta \) is:
\[
\cos\theta = \frac{P}{|S|}
\]
\[
\cos\theta = \frac{40,000}{50,000} = 0.8
\]
Since the load is **delivering a magnetizing reactive power**, that means **inductive** (positive Q). So:
\[
\tan\theta = \frac{Q}{P} = \frac{30,000}{40,000} = 0.75
\]
\[
\theta = \arccos(0.8) \approx 36.87^\circ
\]
---
## **Step 5: Find Resistance and Reactance**
The impedance in polar form:
\[
Z = |Z| \angle \theta = 1.25 \angle 36.87^\circ
\]
In rectangular form:
\[
Z = R + jX
\]
\[
R = |Z| \cos\theta = 1.25 \times 0.8 = 1.0\ \Omega
\]
\[
X = |Z| \sin\theta = 1.25 \times 0.6 = 0.75\ \Omega
\]
---
## **Step 6: Final Answers**
\[
\boxed{
\begin{aligned}
\text{Load Resistance, } R &= 1.0\ \Omega \\
\text{Load Reactance, } X &= 0.75\ \Omega \\
\end{aligned}
}
\]
---
**Summary Table:**
| Quantity | Value |
|-----------------|--------------|
| Resistance (R) | \(1.0~\Omega\) |
| Reactance (X) | \(0.75~\Omega\) |
---
**Explanation:**
- The load absorbs 40 kW (real power) and 30 kVAR (inductive reactive power).
- Apparent power is 50 kVA, so current is 200 A.
- Impedance is 1.25 Ω at 36.87° (power factor angle).
- Convert to rectangular components: \( R = 1.0~\Omega \), \( X = 0.75~\Omega \).
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