Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

A 360 -Hz source of emf is connected in a circuit consisting of a capacitor, a \(25-\mathrm{mH}\) inductor, and an \(0.80-\Omega\) resistor. For the current and the voltage to be in phase, what should the value of \(C\) be?

Short Answer

Expert verified
Answer: The capacitance (C) for the current and voltage to be in phase in the given RLC circuit is approximately 1.246 * 10^-6 F or 1.246 μF.

Step by step solution

01

Given values and formulae

We are given the following values: - Frequency (f) = 360 Hz - Inductor (L) = 25 mH = 0.025 H - Resistor (R) = 0.80 Ω We need to find the capacitance (C) for the current and voltage to be in phase. Formulae we need: 1. Inductive reactance (XL) = 2 * π * f * L 2. Capacitive reactance (XC) = 1 / (2 * π * f * C)
02

Calculate inductive reactance (XL)

Calculate inductive reactance (XL) using the formula: XL = 2 * π * f * L = 2 * π * 360 * 0.025 XL ≈ 56.55 Ω
03

Equate inductive and capacitive reactances

In the case when the current and voltage are in phase, inductive reactance will be equal to capacitive reactance (XL = XC), so we get: 56.55 = 1 / (2 * π * 360 * C)
04

Solve for capacitance (C)

Now rearrange the equation to solve for C: C = 1 / (2 * π * 360 * 56.55) C ≈ 1.246 * 10^-6 F So, the value of the capacitance C should be approximately 1.246 * 10^-6 F or 1.246 μF for the current and voltage to be in phase in the given RLC circuit.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

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.

A 75,000 -W light bulb (yes, there are such things!) operates at \(I_{\mathrm{rms}}=200 . \mathrm{A}\) and \(V_{\mathrm{rms}}=440 . \mathrm{V}\) in a \(60.0-\mathrm{Hz} \mathrm{AC}\) circuit. Find the resistance, \(R,\) and self- inductance, \(L,\) of this bulb. Its capacitive reactance is negligible.

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 series RLC circuit is in resonance when driven by a sinusoidal voltage at its resonant frequency, \(\omega_{0}=(L C)^{-1 / 2} .\) But if the same circuit is driven by a square-wave voltage (which is alternately on and off for equal time intervals), it will exhibit resonance at its resonant frequency and at \(\frac{1}{3}\), \(\frac{1}{5}, \frac{1}{7}, \ldots,\) of this frequency. Explain why.

A series RLC circuit has a source of time-varying emf providing \(12.0 \mathrm{~V}\) at a frequency \(f_{0}\), with \(L=7.00 \mathrm{mH}, R=100 . \Omega\), and \(C=0.0500 \mathrm{mF}\). a) What is the resonant frequency of this circuit? b) What is the average power dissipated in the resistor at this resonant frequency?

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free