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A violin string \(30.0 \mathrm{~cm}\) long with linear density \(0.650 \mathrm{~g} / \mathrm{m}\) is placed near a loudspeaker that is fed by an audio oscillator of variable frequency. It is found that the string is set into oscillation only at the frequencies 880 and \(1320 \mathrm{~Hz}\) as the frequency of the oscillator is varied over the range \(500-1500 \mathrm{~Hz}\). What is the tension in the string?

Short Answer

Expert verified
The tension in the string is 181 N.

Step by step solution

01

Understand the Problem

In this problem, we need to find the tension in a violin string that resonates at frequencies 880 Hz and 1320 Hz. The string has a length of 30.0 cm and a linear density of 0.650 g/m.
02

Identify the Fundamental and Harmonics

The frequencies at which a string vibrates are integral multiples (harmonics) of the fundamental frequency. Here, 1320 Hz (which is equivalent to \(3 \times 440\) Hz) is a harmonic of 880 Hz, indicating 880 Hz is the fundamental frequency (\(f_1\)) and 1320 Hz is the third harmonic (\(f_3\)). Hence, \(f_1 = 880\) Hz.
03

Use Wave Speed and Frequency Relationship

For a string, the wave speed \(v\) is related to the frequency \(f\) and wavelength \(\lambda\) by \(v = f \cdot \lambda\). The wavelength of the fundamental frequency is twice the length of the string, so \(\lambda = 2 \times L = 60.0\) cm or 0.60 m. Therefore, \(v = f_1 \cdot \lambda = 880 \times 0.60\).
04

Calculate the Speed of the Wave

Calculate the wave speed: \(v = 880 \times 0.60 = 528\) m/s. This is the speed of the wave on the string at the fundamental frequency.
05

Relate Wave Speed and Tension

The speed of a wave on a string is given by \(v = \sqrt{T/\mu}\), where \(T\) is the tension and \(\mu\) is the linear density. Rearrange this equation to solve for tension: \(T = v^2 \cdot \mu\).
06

Convert Linear Density

The linear density is given in g/m, but we convert it to kg/m for use in our formula: \(\mu = 0.650 \times 10^{-3}\) kg/m.
07

Calculate the Tension

Substitute \(v = 528\) m/s and \(\mu = 0.650 \times 10^{-3}\) kg/m into the formula for tension: \(T = 528^2 \times 0.650 \times 10^{-3} = 181\) N.

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Key Concepts

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

Harmonics
When you pluck a string, it vibrates at certain frequencies, producing sound waves. Harmonics are these frequencies at which the string naturally resonates. In simple terms, they are specific frequencies that make the string vibrate strongly, creating clear sounds. For any string, the fundamental frequency, also known as the first harmonic, is the lowest frequency at which the string vibrates.
The frequency of each successive harmonic is a whole number multiple of this fundamental frequency. So, if the fundamental frequency is 880 Hz, the second harmonic would be 1760 Hz (2 times the fundamental), and the third harmonic is 1320 Hz (in this case, it's an apparent second because of how the exercise is structured).
Understanding harmonics helps us determine how a string naturally behaves and vibrates, influencing the music we hear. Harmonics are integral in setting the mood and tone of music.
Wave Speed
Wave speed on a string is a measure of how fast the disturbance travels along the string when it's vibrating. It's an important factor because it determines the frequency of sound produced when the string is plucked or played.
  • The wave speed (\(v\)) can be calculated using the formula: \(v = f \cdot \lambda\), where \(f\) is the frequency, and \(\lambda\) is the wavelength of the wave.
  • In a string fixed at both ends, such as a violin string, the wavelength of the fundamental mode is twice the length of the string. Thus, \(\lambda = 2L\).
  • This means that to find wave speed, you multiply the fundamental frequency by twice the string's length.
For example, if the string has a fundamental frequency of 880 Hz and is 0.30 m long, the wave speed calculation would be \(v = 880 \times 2 \times 0.30 = 528\) m/s.
String Tension
String tension refers to the force applied to stretch a string. It's crucial because it affects the pitch of the sound produced. The tighter the string, the higher the pitch because of the increased wave speed.
  • We can calculate string tension (\(T\)) using the formula: \(T = v^2 \cdot \mu\), where \(v\) is the wave speed and \(\mu\) is the linear density.
  • This relationship tells us that tension increases with the square of the wave speed and linearly with the linear density.
In the given problem, with a wave speed of 528 m/s and linear density of 0.650 g/m (converted to kg/m), we calculate the tension as \(T = 528^2 \times 0.650 \times 10^{-3} = 181\) N. This illustrates how tension impacts the frequency at which a string vibrates.
Linear Density
Linear density (\(\mu\)) represents the mass per unit length of the string. It plays a critical role in determining both wave speed and tension for a string.
  • In our context, linear density affects how quickly waves can travel along the string and how much tension is needed to achieve certain pitches.
  • The unit of linear density is usually \(\text{kg/m}\), which helps us in calculations like finding tension using the formula: \(T = v^2 \cdot \mu\).
  • For calculations, ensure the linear density is in the correct unit (e.g., converting from \(\text{g/m}\) to \(\text{kg/m}\)). In our exercise, this conversion was done: \(0.650 \, \text{g/m} = 0.650 \times 10^{-3} \text{kg/m}\).
Understanding linear density gives insight into the structural characteristics of the string, directly influencing sound quality and behavior.

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Most popular questions from this chapter

When you "crack" a knuckle, you suddenly widen the knuckle cavity, allowing more volume for the synovial fluid inside it and causing a gas bubble suddenly to appear in the fluid. The sudden production of the bubble, called "cavitation," produces a sound pulse \(-\) the cracking sound. Assume that the sound is transmitted uniformly in all directions and that it fully passes from the knuckle interior to the outside. If the pulse has a sound level of \(62 \mathrm{~dB}\) at your ear, estimate the rate at which energy is produced by the cavitation.

At a certain point, two waves produce pressure variations given by \(\Delta p_{1}=\Delta p_{m} \sin \omega t\) and \(\Delta p_{2}=\Delta p_{m} \sin (\omega t-\phi) .\) At this point, what is the ratio \(\Delta p_{r} / \Delta p_{m},\) where \(\Delta p_{r}\) is the pressure amplitude of the resultant wave, if \(\phi\) is (a) \(0,\) (b) \(\pi / 2,\) (c) \(\pi / 3\), and (d) \(\pi / 4 ?\)

A pipe \(0.60 \mathrm{~m}\) long and closed at one end is filled with an unknown gas. The third lowest harmonic frequency for the pipe is \(750 \mathrm{~Hz}\). (a) What is the speed of sound in the unknown gas? (b) What is the fundamental frequency for this pipe when it is filled with the unknown gas?

You are standing at a distance \(D\) from an isotropic point source of sound. You walk \(50.0 \mathrm{~m}\) toward the source and observe that the intensity of the sound has doubled. Calculate the distance \(D\).

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