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

The middle-C key (key 52 ) on a piano corresponds to a fundamental frequency of about \(262 \mathrm{~Hz},\) and the sopranoC key (key 64) corresponds to a fundamental frequency of \(1046.5 \mathrm{~Hz}\). If the strings used for both keys are identical in density and length, determine the ratio of the tensions in the two strings.

Short Answer

Expert verified
Answer: The ratio of tensions in the two strings is 1:16.

Step by step solution

01

Write the fundamental frequency formula for both keys

To find the ratio of the tensions of the two strings, first write the fundamental frequency formula for each of the keys (middle-C and soprano-C): Middle-C key: \(f_{1} = \frac{1}{2L} \sqrt{\frac{T_{1}}{\mu}}\) Soprano-C key: \(f_{2} = \frac{1}{2L} \sqrt{\frac{T_{2}}{\mu}}\)
02

Set up a proportion to compare the two strings

Since the two strings have the same density and length, the ratio of their fundamental frequencies should be proportional to the ratio of their tensions. We can write this proportion as: \(\frac{f_{1}}{f_{2}} = \frac{\frac{1}{2L} \sqrt{\frac{T_{1}}{\mu}}}{\frac{1}{2L} \sqrt{\frac{T_{2}}{\mu}}}\) Here, \(f_{1} = 262 \mathrm{~Hz}\) (middle-C frequency) and \(f_{2} = 1046.5 \mathrm{~Hz}\) (soprano-C frequency).
03

Simplify the proportion and solve for the tension ratio

Next, simplify the proportion: \(\frac{262}{1046.5} = \frac{\sqrt{\frac{T_{1}}{\mu}}}{\sqrt{\frac{T_{2}}{\mu}}}\) Square both sides of the equation to get rid of the square roots: \(\left(\frac{262}{1046.5}\right)^{2} = \frac{\frac{T_{1}}{\mu}}{\frac{T_{2}}{\mu}}\) Now, multiply both sides by \(T_{2}\) to isolate the ratio \(\frac{T_{1}}{T_{2}}\): \(\frac{T_{1}}{T_{2}} = \left(\frac{262}{1046.5}\right)^{2} \cdot 1\)
04

Calculate the tension ratio

Finally, calculate the tension ratio: \(\frac{T_{1}}{T_{2}} = \left(\frac{262}{1046.5}\right)^{2}\) \(\frac{T_{1}}{T_{2}} = \frac{1}{16}\) So, the ratio of the tensions in the two strings is \(1:16\).

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.

Fundamental Frequency
The fundamental frequency is a crucial concept in the world of sound and vibration. It refers to the lowest frequency produced by any vibrating object, like a string or a column of air. The fundamental frequency determines the pitch of the sound, making it an essential element in music and acoustics.
To calculate the fundamental frequency of a string, we use the formula:
  • \( f = \frac{1}{2L} \sqrt{\frac{T}{\mu}} \)

    Where:

    • \(f\) is the fundamental frequency,
    • \(L\) is the length of the string,
    • \(T\) is the tension in the string,
    • \(\mu\) is the linear mass density of the string.
This equation shows how the fundamental frequency is influenced by string length, tension, and density. Higher tension results in higher frequencies, while greater density or length lowers the frequency. Understanding this relationship helps in designing and playing musical instruments like pianos.
Piano Physics
The physics of a piano involves the transformation of mechanical energy into sound energy. When a key on a piano is struck, it causes a hammer to hit a string inside the piano. This action makes the string vibrate, producing sound waves that we hear as music.
Pianos use different strings of varying lengths, tensions, and densities to produce a wide range of notes. For instance:
  • Lower notes are produced by longer and thicker strings, which vibrate more slowly.
  • Higher notes come from shorter, thinner strings, which vibrate at a faster rate.
Each string is tuned to a specific tension to achieve its intended pitch. The keys, hammers, and strings work together in harmony, guided by principles of physics, to create the piano's distinctive sound. Musicians leverage their understanding of these mechanics to master their instrument and produce beautiful music.
String Density
String density, or linear mass density, is a measure of how much mass a string has per unit length. It's denoted by the symbol \(\mu\) and is a fundamental property influencing a string's vibration characteristics.
The string density affects the sound produced by an instrument in several ways:
  • Thicker, denser strings tend to produce lower-pitched sounds, as they have more mass per unit length, causing them to vibrate more slowly.
  • Lighter, less dense strings vibrate more quickly, resulting in higher-pitched sounds.
The density of a string is as important as its length and tension when it comes to determining its fundamental frequency. For a given tension and length, increasing the density will lower the frequency of the sound produced.
In the study of a piano's middle-C and soprano-C keys, the density remains constant, allowing us to focus on tension differences to understand frequency changes.
Wave Equations
Wave equations are mathematical expressions that describe the behavior of waves as they travel through different mediums, like strings or air. In the context of stringed instruments like the piano, wave equations help us understand how strings vibrate to produce sound.
For a vibrating string, the wave equation is expressed as:\[\frac{\partial^2 y}{\partial t^2} = v^2 \frac{\partial^2 y}{\partial x^2}\]Here:
  • \(y\) represents the displacement of the string at a point and time.
  • \(v\) is the wave speed, dependent on the tension and density of the string.
Solving this wave equation gives insight into how waves propagate along the string, affecting its frequency and the sound emitted. Understanding these equations allows musicians and instrument makers to manipulate variables like string tension and length to achieve the desired tones.
In the problem of determining string tension ratios, wave equations facilitate the correlation between physical properties and sound frequencies, providing a mathematical framework for music acoustics.

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

The speed of light waves in air is greater than the speed of sound in air by about a factor of a million. Given a sound wave and a light wave of the same wavelength, both traveling through air, which statement about their frequencies is true? a) The frequency of the sound wave will be about a million times greater than that of the light wave. b) The frequency of the sound wave will be about a thousand times greater than that of the light wave. c) The frequency of the light wave will be about a thousand times greater than that of the sound wave. d) The frequency of the light wave will be about a million times greater than that of the sound wave. e) There is insufficient information to determine the relationship between the two frequencies.

What is the wave speed along a brass wire with a radius of \(0.500 \mathrm{~mm}\) stretched at a tension of \(125 \mathrm{~N}\) ? The density of brass is \(8.60 \cdot 10^{3} \mathrm{~kg} / \mathrm{m}^{3}\).

Suppose that the tension is doubled for a string on which a standing wave is propagated. How will the velocity of the standing wave change? a) It will double. c) It will be multiplied by \(\sqrt{2}\). b) It will quadruple. d) It will be multiplied by \(\frac{1}{2}\).

a) Starting from the general wave equation (equation 15.9 ), prove through direct derivation that the Gaussian wave packet described by the equation \(y(x, t)=(5.00 m) e^{-0.1(x-5 t)^{2}}\) is indeed a traveling wave (that it satisfies the differential wave equation). b) If \(x\) is specified in meters and \(t\) in seconds, determine the speed of this wave. On a single graph, plot this wave as a function of \(x\) at \(t=0, t=1.00 \mathrm{~s}, t=2.00 \mathrm{~s},\) and \(t=3.00 \mathrm{~s}\) c) More generally, prove that any function \(f(x, t)\) that depends on \(x\) and \(t\) through a combined variable \(x \pm v t\) is a solution of the wave equation, irrespective of the specific form of the function \(f\)

The different colors of light we perceive are a result of the varying frequencies (and wavelengths) of the electromagnetic radiation. Infrared radiation has lower frequencies than does visible light, and ultraviolet radiation has higher frequencies than visible light does. The primary colors are red (R), yellow (Y), and blue (B). Order these colors by their wavelength, shortest to longest. a) \(\mathrm{B}, \mathrm{Y}, \mathrm{R}\) b) \(B, R, Y\) c) \(\mathrm{R}, \mathrm{Y}, \mathrm{B}\) d) \(R, B, Y\)

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