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A series RLC circuit attached to a \(120 \mathrm{V} / 60 \mathrm{Hz}\) power line draws 2.4 A of current with a power factor of \(0.87 .\) What is the value of the resistor?

Short Answer

Expert verified
The value of the resistor is approximately \(43.68 \Omega\).

Step by step solution

01

Find the Apparent Power (S)

The current drawn from the supply is 2.4A and the voltage is 120V. Using these values, calculate the apparent power (S) which is the product of the Voltage (V) and the Current (I). So, \(S = VI = 2.4A*120V = 288 VA.\)
02

Calculate the Real Power (P)

Real power (P) is the product of the apparent power (S) and the power factor (PF). Here, S is 288 VA and the PF is given as 0.87. Calculate the real power as follows: \(P = S \cdot PF = 288VA * 0.87 = 250.56 W.\)
03

Find the Resistance (R)

The resistance (R) can be found by using the formula for power in resistive circuits, which is \(P = I^2R\), where P is the real power, I is the current, and R is the resistance. Rearrange the formula to solve for R: \(R = P/I^2 = 250.56W / (2.4A)^2 = 43.68 \Omega.\)

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Apparent Power
When dealing with electrical circuits, especially those involving alternating current (AC), it is important to understand the concept of apparent power. Apparent power, denoted as \( S \), essentially represents the product of the circuit's voltage and current. It is measured in Volt-Amperes (VA) and gives a combined idea of what the circuit could deliver in power, without differentiating whether this power does actual work or not.
For our given problem, the apparent power calculation seems straightforward. You take the 120V voltage across the circuit and multiply it by the 2.4A current flowing through it:
  • Voltage \( (V) = 120 \text{V} \)
  • Current \( (I) = 2.4 \text{A} \)
  • Apparent Power \( (S) = V \cdot I = 120 \times 2.4 = 288 \text{VA} \)
This number, 288 VA, tells us the potential energy transferred from the source to the circuit. However, not all of this power is usable for work since it combines both useful (real) power and non-useful (reactive) power components.
Real Power
Real power is the portion of apparent power that actually performs work in the circuit. This is the power that is converted into heat, light, motion, etc. The unit for real power is Watts (W).
The relationship between real and apparent power is heavily influenced by the power factor \( (PF) \), which measures how effectively the current is being converted into useful work. To calculate real power \( (P) \), we adjust the apparent power by the power factor:
  • Apparent Power \( (S) = 288 \text{VA} \)
  • Power Factor \( (PF) = 0.87 \)
  • Real Power \( (P) = S \times PF = 288 \times 0.87 = 250.56 \text{W} \)
The formula shows us that out of the 288 VA available, 250.56 W is actually being put to useful work in the circuit.
Power Factor
The power factor is a key element in AC circuit analysis that indicates the ratio of real power used in a circuit to the apparent power drawn from the source. Expressed as a decimal or percentage, the power factor describes how effectively electrical power is being used.
A power factor of 1 (or 100%) is ideal as it means all the supplied power is being converted into useful work. In our problem, we have a power factor of 0.87, which suggests a good efficiency but some inefficiency is loaded by the reactive components of the circuit:
- **Inductive or capacitive components** cause the waveform of current to lag or lead the voltage waveform. - **The closer the power factor to 1**, the more effective the circuit is.
Thus, improving power factor often leads to reduced energy losses and improved voltage regulation in power systems.
Resistance Calculation
In any electrical circuit, finding the resistance is crucial for understanding how the circuit functions. Resistance \( (R) \) in an RLC circuit can be determined using measurements of real power and current.
From Ohm's Law and the formula for power in resistive components, we can use the formula:
\[ P = I^2R \]
Where:
  • \( P \) is the real power (250.56 W)
  • \( I \) is the current (2.4 A)
We rearrange it for resistance:
  • \( R = \frac{P}{I^2} = \frac{250.56}{2.4^2} = 43.68 \Omega \)
This resistance value describes how much the circuit opposes the flow of current, affecting the overall energy efficiency of the electrical setup.

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Most popular questions from this chapter

A 200 \(\Omega\) resistor is connected to an AC source with \(\mathcal{E}_{0}=10 \mathrm{V} .\) What is the peak current through the resistor if the emf frequency is (a) \(100 \mathrm{Hz} ?\) (b) \(100 \mathrm{kHz} ?\)

Commercial electricity is generated and transmitted as threephase electricity. Instead of a single emf \(\mathcal{E}=\mathcal{E}_{0} \cos \omega t\), three separate wires carry currents for the emfs \(\mathcal{E}_{1}=\mathcal{E}_{0} \cos \omega t\) \(\mathcal{E}_{2}=\mathcal{E}_{0} \cos \left(\omega t+120^{\circ}\right),\) and \(\mathcal{E}_{3}=\mathcal{E}_{0} \cos \left(\omega t-120^{\circ}\right) .\) This is why the long-distance transmission lines you see in the countryside have three parallel wires, as do many distribution lines within a city. a. Draw a phasor diagram showing phasors for all three phases of a three-phase emf. b. Show that the sum of the three phases is zero, producing what is referred to as neutral. In single-phase electricity, provided by the familiar \(120 \mathrm{V} / 60 \mathrm{Hz}\) electric outlets in your home, one side of the outlet is neutral, as established at a nearby electrical substation. The other, called the hot side, is one of the three phases. (The round opening is connected to ground.) c. Show that the potential difference between any two of the phases has the rms value \(\sqrt{3} \mathcal{E}_{\text {rms }},\) where \(\mathcal{E}_{\text {rms }}\) is the familiar single-phase rms voltage. Evaluate this potential difference for \(\mathcal{E}_{\text {rms }}=120 \mathrm{V}\) Some high-power home appliances, especially electric clothes dryers and hot-water heaters, are designed to operate between two of the phases rather than between one phase and neutral. Heavy-duty industrial motors are designed to operate from all three phases, but full three phase power is rare in residential or office use.

a. Show that the peak inductor voltage in a series \(R L C\) circuit is maximum at frequency $$\omega_{\mathrm{L}}=\left(\frac{1}{\omega_{0}^{2}}-\frac{1}{2} R^{2} C^{2}\right)^{-1 / 2}$$ b. A series RLC circuit with \(\mathcal{E}_{0}=10.0 \mathrm{V}\) consists of a \(1.0 \Omega\) resistor, a \(1.0 \mu \mathrm{H}\) inductor, and a \(1.0 \mu \mathrm{F}\) capacitor. What is \(V_{\mathrm{L}}\) at \(\omega=\omega_{0}\) and at \(\omega=\omega_{L} ?\)

Commercial electricity is generated and transmitted as three phase electricity. Instead of a single emf, three separate wires carry currents for the emfs \(\mathcal{E}_{1}=\mathcal{E}_{0} \cos \omega t, \mathcal{E}_{2}=\mathcal{E}_{0} \cos (\omega t+\) \(\left.120^{\circ}\right),\) and \(\mathcal{E}_{3}=\mathcal{E}_{0} \cos \left(\omega t-120^{\circ}\right)\) over three parallel wires, each of which supplies one-third of the power. This is why the long-distance transmission lines you see in the countryside have three wires. Suppose the transmission lines into a city supply a total of 450 MW of electric power, a realistic value. a. What would be the current in each wire if the transmission voltage were \(\mathcal{E}_{0}=120 \mathrm{V} \mathrm{rms} ?\) b. In fact, transformers are used to step the transmission-line voltage up to \(500 \mathrm{kV}\) ms. What is the current in each wire? c. Big transformers are expensive. Why does the electric company use step-up transformers?

A low-pass filter consists of a \(100 \mu \mathrm{F}\) capacitor in series with a \(159 \Omega\) resistor. The circuit is driven by an AC source with a peak voltage of \(5.00 \mathrm{V}\) a. What is the crossover frequency \(f_{c} ?\) b. What is \(V_{\mathrm{C}}\) when \(f=\frac{1}{2} f_{\mathrm{c}}, f_{\mathrm{c}},\) and \(2 f_{\mathrm{c}} ?\)

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