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 string is \(35.0 \mathrm{~cm}\) long and has a mass per unit length of \(5.51 \cdot 10^{-4} \mathrm{~kg} / \mathrm{m} .\) What tension must be applied to the string so that it vibrates at the fundamental frequency of \(660 . \mathrm{Hz?}\)

Short Answer

Expert verified
Answer: The tension required is approximately 56.753 N.

Step by step solution

01

Convert string length to meters

The given length of the string is 35.0 cm, but we need it to be in meters to be consistent with units in the formula. To convert to meters, divide by 100: $$ L = \frac{35.0 \ \mathrm{cm}}{100} = 0.35 \ \mathrm{m} $$
02

Write down the known values

Using the converted length, we now list the known values: - Length of string, \(L = 0.35 \ \mathrm{m}\) - Mass per unit length of the string, \(\mu = 5.51*10^{-4} \ \mathrm{kg/m}\) - Fundamental frequency, \(f = 660 \ \mathrm{Hz}\)
03

Rearrange the formula to solve for tension

Rearrange the formula for the fundamental frequency to solve for the tension \(T\): $$ T = \mu \left(2L f\right)^2 $$
04

Plug in values and solve for tension

Now, we can plug in the known values into the formula and solve for \(T\): $$ T = \left(5.51 * 10^{-4} \ \mathrm{kg/m}\right) \left(2 * 0.35 \ \mathrm{m} * 660 \ \mathrm{Hz}\right)^2 $$ Calculate the tension: $$ T \approx 56.753 \ \mathrm{N} $$ The tension required to make the string vibrate at the fundamental frequency of 660 Hz is approximately 56.753 N.

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!

Key Concepts

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

String Tension Calculation
The ability to calculate the tension in a vibrating string is crucial for understanding a wide range of musical and physical phenomena. When a string is plucked or struck, the tension contributes to its vibrational properties, which in turn determine the pitch of the sound produced. To find out the necessary tension to achieve a particular frequency, we use the formula connecting tension (T), mass per unit length (\textbf{\textmu}), and frequency (f):

\textbf{Formula for Tension:} \[ T = \textbf{\textmu} (2Lf)^2 \]
Surprisingly, this formula shows that the tension increases with the square of the frequency, highlighting how dramatically tension must change to reach higher pitches. In our exercise, the result was approximately 56.753 Newtons (N). Understanding string tension is important not only for musicians tuning their instruments but also for engineers and physicists dealing with materials and resonances.
Mass Per Unit Length
Mass per unit length (often denoted as \textbf{\textmu}) is a fundamental property of strings that directly affects their vibrational characteristics. It is defined as the mass of the string divided by its length:

\textbf{Definition:} \[ \textbf{\textmu} = \frac{\text{Mass}}{\text{Length}} \]
This property is key to determining the string’s inertia and resistance to acceleration during vibration. A higher mass per unit length implies a slower response to force, resulting in a lower pitch, while a lower mass per unit length allows for higher frequencies. In the given exercise, we used the value of \( 5.51 \times 10^{-4} \text{ kg/m} \) to calculate the tension needed for a specific vibrational frequency. When designers craft musical instruments, such as guitars or pianos, they carefully consider the mass per unit length to ensure the instrument can produce the desired range of notes.
Harmonics in Physics
Harmonics, or overtones, are an essential concept in physics, explaining the phenomenon of multiples of a fundamental frequency. When a string vibrates, it doesn't just produce one single note but also generates a series of higher-pitched sounds at frequencies that are integer multiples of the fundamental frequency (f).

\textbf{Harmonic Series:} \[ f_n = n \times f \]
Here, \( f_n \) represents the frequency of the nth harmonic, and n is an integer. The first harmonic (n=1) is the fundamental frequency, the second harmonic (n=2) is twice the fundamental, and so forth. This series enriches the sound produced by musical instruments and is also a cornerstone in understanding complex waveforms. The understanding of harmonics not only aids in music theory and instrumentation but is also pivotal in areas such as acoustics, electronics, and even telecommunications.

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

Noise results from the superposition of a very large number of sound waves of various frequencies (usually in a continuous spectrum), amplitudes, and phases. Can interference arise with noise produced by two sources?

A rubber band of mass \(0.3491 \mathrm{~g}\) is stretched between two fingers, putting each side under a tension of \(1.777 \mathrm{~N}\). The overall stretched length of the band is \(20.27 \mathrm{~cm} .\) One side of the band is plucked, setting up a vibration in \(8.725 \mathrm{~cm}\) of the band's stretched length. What is the lowest-frequency vibration that can be set up on this part of the rubber band? Assume that the band stretches uniformly.

A sinusoidal transverse wave of wavelength \(20.0 \mathrm{~cm}\) and frequency 500\. Hz travels along a string in the positive \(z\) -direction. The wave oscillations take place in the \(x z\) -plane and have an amplitude of \(3.00 \mathrm{~cm}\). At time \(t=0,\) the displacement of the string at \(x=0\) is \(z=3.00 \mathrm{~cm}\) a) A photo of the wave is taken at \(t=0 .\) Make a simple sketch (including axes) of the string at this time. b) Determine the speed of the wave. c) Determine the wave's wave number. d) If the linear mass density of the string is \(30.0 \mathrm{~g} / \mathrm{m},\) what is the tension in the string? e) Determine the function \(D(z, t)\) that describes the displacement \(x\) that is produced in the string by this wave.

In an acoustics experiment, a piano string with a mass of \(5.00 \mathrm{~g}\) and a length of \(70.0 \mathrm{~cm}\) is held under tension by running the string over a frictionless pulley and hanging a \(250 .-\mathrm{kg}\) weight from it. The whole system is placed in an elevator. a) What is the fundamental frequency of oscillation for the string when the elevator is at rest? b) With what acceleration and in what direction (up or down) should the elevator move for the string to produce the proper frequency of \(440 . \mathrm{Hz}\) corresponding to middle A?

A particular steel guitar string has a mass per unit length of \(1.93 \mathrm{~g} / \mathrm{m}\). a) If the tension on this string is \(62.2 \mathrm{~N},\) what is the wave speed on the string? b) For the wave speed to be increased by \(1.00 \%\), how much should the tension be changed?

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