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At what frequency will a \(10.0-\mu \mathrm{F}\) capacitor have reactance \(X_{C}=200 . \Omega ?\)

Short Answer

Expert verified
Answer: The frequency at which the 10.0 µF capacitor will have a reactance of 200 Ω is approximately 7957.75 Hz.

Step by step solution

01

Write down the given values and formula

We are given the values for capacitive reactance (X_C) and capacitance (C). Write down these values: Capacitive Reactance, \(X_{C} = 200 \Omega\) Capacitance, \(C = 10.0 \times 10^{-6} \mathrm{F}\) We will use the formula for capacitive reactance to solve for the frequency (f): \(X_{C} = \frac{1}{2 \pi f C}\)
02

Solve the equation for frequency (f)

Rearrange the formula to solve for frequency (f): \(f = \frac{1}{2 \pi X_{C} C}\)
03

Substitute the given values and calculate frequency (f)

Plug in the given values of X_C and C into the equation: \(f = \frac{1}{2 \pi (200 \Omega)(10.0 \times 10^{-6} \mathrm{F})}\) Now, calculate the frequency (f): \(f \approx 7957.75 \mathrm{Hz}\)
04

Write the final answer

The frequency at which the \(10.0-\mu \mathrm{F}\) capacitor will have a reactance of \(200 . \Omega\) is approximately \(7957.75 \mathrm{Hz}\).

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Key Concepts

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

Capacitive Reactance
Capacitive reactance is a measure of how much a capacitor resists the flow of alternating current (AC). It is denoted by the symbol \(X_C\) and is measured in ohms (\(\Omega\)). Unlike resistance, which applies to direct current (DC), capacitance reactance only comes into play with AC.
The capacitive reactance decreases as the frequency of the AC increases, because the capacitor will "charge" and "discharge" more quickly.
  • High Frequency = Lower Reactance: At higher frequencies, electrons switch direction more often, causing the capacitor to "fill" and "empty" faster.
  • Low Frequency = Higher Reactance: Fewer cycles per second mean that the capacitor charges slower, offering more opposition to the flow.
This concept is crucial in designing circuits, as it helps control how much current flows at different frequencies.
Frequency
In the context of electric circuits, frequency refers to how often the current changes direction each second. It is measured in Hertz (Hz), where 1 Hz means one cycle per second.
Frequency plays a big role in determining the performance of AC circuits. Higher frequencies cause reactance to decrease, while lower frequencies increase reactance.
For a capacitor like the one in the exercise, higher frequencies will allow more current to pass through due to lower reactance.
  • Frequency is inversely related to reactance: As frequency increases, reactance decreases.
  • A balance between frequency and capacitance is essential for controlling the amount of AC that can pass through a circuit.
Formula Derivation
To find out how capacitive reactance relates to frequency and capacitance, the formula derived is \(X_C = \frac{1}{2\pi f C}\). This shows how reactance is inversely proportional to both frequency (\(f\)) and capacitance (\(C\)).
We can reformulate this to solve for frequency when we know the reactance and capacitance:
  • Start with the formula: \(X_C = \frac{1}{2\pi f C}\)
  • Rearrange to solve for frequency: \(f = \frac{1}{2\pi X_C C}\)
By plugging in the values from the exercise \(X_C = 200 \Omega\) and \(C = 10.0 \times 10^{-6} F\), we calculate the frequency:
  • Use the rearranged formula: \(f \approx 7957.75 \text{ Hz}\)
This derived formula helps customize circuits for specific frequencies by adjusting capacitance and measuring reactance, making it a powerful tool in electronics and engineering.

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Most popular questions from this chapter

When you turn the dial on a radio to tune it, you are adjusting a variable capacitor in an LC circuit. Suppose you tune to an AM station broadcasting at a frequency of \(1000 . \mathrm{kHz},\) and there is a \(10.0-\mathrm{mH}\) inductor in the tuning circuit. When you have tuned in the station, what is the capacitance of the capacitor?

A common configuration of wires has twisted pairs as opposed to straight, parallel wires. What is the technical advantage of using twisted pairs of wires versus straight, parallel pairs?

A transformer has 800 turns in the primary coil and 40 turns in the secondary coil. a) What happens if an AC voltage of \(100 . \mathrm{V}\) is across the primary coil? b) If the initial \(A C\) current is \(5.00 \mathrm{~A}\), what is the output current? c) What happens if a DC current at \(100 .\) V flows into the primary coil? d) If the initial DC current is \(5.00 \mathrm{~A}\), what is the output current?

Laboratory experiments with series RLC circuits require some care, as these circuits can produce large voltages at resonance. Suppose you have a 1.00 - \(\mathrm{H}\) inductor (not difficult to obtain) and a variety of resistors and capacitors. Design a series RLC circuit that will resonate at a frequency (not an angular frequency) of \(60.0 \mathrm{~Hz}\) and will produce at resonance a magnification of the voltage across the capacitor or the inductor by a factor of 20.0 times the input voltage or the voltage across the resistor.

The figure shows a simple FM antenna circuit in which \(L=8.22 \mu \mathrm{H}\) and \(C\) is variable (the capacitor can be tuned to receive a specific station). The radio signal from your favorite FM station produces a sinusoidal time-varying emf with an amplitude of \(12.9 \mu \mathrm{V}\) and a frequency of \(88.7 \mathrm{MHz}\) in the antenna. a) To what value, \(C_{0}\), should you tune the capacitor in order to best receive this station? b) Another radio station's signal produces a sinusoidal time-varying emf with the same amplitude, \(12.9 \mu \mathrm{V}\), but with a frequency of \(88.5 \mathrm{MHz}\) in the antenna. With the circuit tuned to optimize reception at \(88.7 \mathrm{MHz}\), what should the value, \(R_{0}\), of the resistance be in order to reduce by a factor of 2 (compared to the current if the circuit were optimized for \(88.5 \mathrm{MHz}\) ) the current produced by the signal from this station?

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