/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 52 You are designing a two-string i... [FREE SOLUTION] | 91Ó°ÊÓ

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You are designing a two-string instrument with metal strings \(35.0 \mathrm{~cm}\) long, as shown in Fig. \(\mathrm{P} 15.52 .\) Both strings are under the same tension. String \(S_{1}\) has a mass of \(8.00 \mathrm{~g}\) and produces the note middle \(\mathrm{C}\) (frequency \(262 \mathrm{~Hz}\) ) in its fundamental mode. (a) What should be the tension in the string? (b) What should be the mass of string \(S_{2}\) so that it will produce A-sharp (frequency \(466 \mathrm{~Hz}\) ) as its fundamental? (c) To extend the range of your instrument, you include a fret located just under the strings but not normally touching them. How far from the upper end should you put this fret so that when you press \(S_{1}\) tightly against it, this string will produce \(\mathrm{C}\) -sharp (frequency \(277 \mathrm{~Hz}\) ) in its fundamental? That is, what is \(x\) in the figure? (d) If you press \(S_{2}\) against the fret, what frequency of sound will it produce in its fundamental?

Short Answer

Expert verified
The tension in the string is approximately 79.69 N. The mass of string S2 should be approximately 15 g. The fret should be placed approximately 3.2 cm from the upper end to produce C-sharp on string S1. When S2 is pressed against the fret, it will produce a frequency of approximately 501 Hz.

Step by step solution

01

Calculate the tension in string S1

Use the formula \(f = \frac{1}{2L}\sqrt{\frac{T}{\mu}}\) to compute the tension \(T\). First, calculate the linear density \(\mu\) of the string, using the given mass and length. \(\mu = \frac{mass}{length} = \frac{8.00g}{35.0cm} = 0.22857 g/cm = 228.57 g/m\). Now, rearrange the formula to solve for \(T\): \(T = (f * 2L)^2 * \mu\).Substitute the known values: \(T = (262Hz * 2*0.35m)^2 * 228.57 g/m = 79.69 N\).
02

Calculate the mass of string S2

The problem states that string S2 is under the same tension and same length as string S1, but produces a different fundamental frequency. Thus, its linear density must differ.First, rearrange the formula to solve for \(\mu\) this time: \(\mu = \frac{(f * 2L)^2}{T}\).Substitute the known values for \(f = 466 Hz\), \(L = 0.35 m\), \(T = 79.69 N\). We find \(\mu = 0.41736 kg/m\).Now, convert \(\mu\) back to mass by multiplying with length: \(mass = \mu * length = 0.41736 kg/m * 0.35 m = 0.015 kg = 15g\).
03

Calculate the location of the fret for string S1 to produce C-sharp

Pressing the fret on string S1 changes the effective vibrating length of the string. We need to find this new length (\(L'\)) for when the string produces the note C-sharp (frequency 277 Hz). Use the formula for fundamental frequency, but this time solve for \(L'\): \(L' = \frac{1}{2f}\sqrt{\frac{T}{\mu}}\).Substitute the known values for \(T\), \(f\), and \(\mu\) and solve to find \(L' = 0.318 m\).Now, the location of the fret (\(x\)) is given by \(x = L - L'\) = 0.35m - 0.318m = 0.032m = 3.2cm.
04

Calculate the new frequency produced by string S2 when pressed against the fret

The problem asks for the new fundamental frequency when string S2 is pressed against the fret at location \(x\). Since the effective length of string S2 is now also \(L'\), we can again use \(f = \frac{1}{2L'}\sqrt{\frac{T}{\mu}}\) to solve for the new frequency.Substitute the known values: \(f' = \frac{1}{2*0.318m}\sqrt{\frac{79.69N}{0.41736 kg/m}} = 501 Hz.\)

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Key Concepts

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

Tension in Strings
The tension in a string has a direct influence on the frequency of the sound wave that the string produces when it is vibrated. Tension is the force stretching the string, and it's measured in units of newtons (N). In musical instruments, increasing the tension typically raises the pitch of the note produced by making the vibrations faster.

For instance, when designing a string instrument, the string must be tight enough to vibrate at a certain fundamental frequency. In this example, string S1 is tuned to produce the middle C note which has a frequency of 262 Hz. By using the formula \(f = \frac{1}{2L}\sqrt{\frac{T}{\mu}}\), we can calculate the tension needed for this frequency when we know the vibrating string length and its linear density. The resultant high tension ensures the string vibrates at the required frequency, creating the desired pitch.
Linear Density of String
Linear density, symbolized by \(\mu\), is the measure of mass per unit length of a string and is expressed in units like grams per meter (g/m). It plays a critical role in determining the frequency of the sound wave produced by a string. The linear density along with tension and the length of the string dictates the rate at which the string will vibrate.

To find the mass of string S2 for our two-string instrument, we need to first calculate its linear density so that it will produce an A-sharp when vibrating. Once we've found the value \(\mu\), we can find the mass by multiplying the linear density by the length of the string. It's a step involving straightforward calculation, nonetheless vital for ensuring the string produces the intended note.
Frequency of Sound Wave
The frequency of a sound wave is directly related to the pitch of the sound we hear. It is measured in Hertz (Hz) and represents the number of vibrations per second. For a string instrument, when the string vibrates in its fundamental mode, the frequency is at its lowest value for that particular length and tension.

The known frequencies of musical notes allow us to design instruments with precision. Middle C has a frequency of 262 Hz, while A-sharp has a frequency of 466 Hz. Using the formula mentioned before, we rearrange it based on what we need to find, whether it is the tension for a known frequency or a frequency that will be produced by adjusting the tension or the length of the string. Subsequently, each variation requires a new calculation to ensure the correct note is produced.
Vibrating String Length
The length of a vibrating string determines the wavelengths of the sound waves it produces, which in turn affects the frequency and pitch of the sound. By adjusting the length of the string using a fret, as in the given exercise, we can alter the pitch it produces without changing the tension.

For example, when the fret is pressed against string S1 to produce a C-sharp note at a frequency of 277 Hz, this changes the effective vibrating length. Here we have calculated this new length (\(L'\)) using the same equation for fundamental frequency, but we rearranged it to solve for the new length based on the desired frequency. By controlling the vibrating string length, we enable the instrument to produce a variety of notes and extend its playable range.

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Most popular questions from this chapter

A transverse sine wave with an amplitude of \(2.50 \mathrm{~mm}\) and a wavelength of \(1.80 \mathrm{~m}\) travels from left to right along a long, horizontal, stretched string with a speed of \(36.0 \mathrm{~m} / \mathrm{s}\). Take the origin at the left end of the undisturbed string. At time \(t=0\) the left end of the string has its maximum upward displacement. (a) What are the frequency, angular frequency, and wave number of the wave? (b) What is the function \(y(x, t)\) that describes the wave? (c) What is \(y(t)\) for a particle at the left end of the string? (d) What is \(y(t)\) for a particle \(1.35 \mathrm{~m}\) to the right of the origin? (e) What is the maximum magnitude of transverse velocity of any particle of the string? (f) Find the transverse displacement and the transverse velocity of a particle \(1.35 \mathrm{~m}\) to the right of the origin at time \(t=0.0625 \mathrm{~s}\)

In your physics lab, an oscillator is attached to one end of a horizontal string. The other end of the string passes over a frictionless pulley. You suspend a mass \(M\) from the free end of the string, producing tension \(M g\) in the string. The oscillator produces transverse waves of frequency \(f\) on the string. You don't vary this frequency during the experiment, but you try strings with three different linear mass densities \(\mu .\) You also keep a fixed distance between the end of the string where the oscillator is attached and the point where the string is in contact with the pulley's rim. To produce standing waves on the string, you vary \(M ;\) then you measure the node-to-node distance \(d\) for each standing-wave pattern and obtain the following data: $$ \begin{array}{l|lllll} \text { String } & \text { A } & \text { A } & \text { B } & \text { B } & \text { C } \\ \hline \mu(\mathrm{g} / \mathrm{cm}) & 0.0260 & 0.0260 & 0.0374 & 0.0374 & 0.0482 \\ M(\mathrm{~g}) & 559 & 249 & 365 & 207 & 262 \\ d(\mathrm{~cm}) & 48.1 & 31.9 & 32.0 & 24.2 & 23.8 \end{array} $$ (a) Explain why you obtain only certain values of \(d\). (b) Graph \(\mu d^{2}(\) in \(\mathrm{kg} \cdot \mathrm{m})\) versus \(M(\) in \(\mathrm{kg}) .\) Explain why the data plotted this way should fall close to a straight line. (c) Use the slope of the best straightline fit to the data to determine the frequency \(f\) of the waves produced on the string by the oscillator. Take \(g=9.80 \mathrm{~m} / \mathrm{s}^{2}\). (d) For string A \((\mu=0.0260 \mathrm{~g} / \mathrm{cm}),\) what value of \(M\) (in grams) would be required to produce a standing wave with a node-to-node distance of \(24.0 \mathrm{~cm}\) ? Use the value of \(f\) that you calculated in part (c).

For a string stretched between two supports, two successive standing-wave frequencies are \(525 \mathrm{~Hz}\) and \(630 \mathrm{~Hz}\). There are other standing-wave frequencies lower than \(525 \mathrm{~Hz}\) and higher than \(630 \mathrm{~Hz}\). If the speed of transverse waves on the string is \(384 \mathrm{~m} / \mathrm{s},\) what is the length of the string? Assume that the mass of the wire is small enough for its effect on the tension in the wire to be ignored.

A string with both ends held fixed is vibrating in its third harmonic. The waves have a speed of \(192 \mathrm{~m} / \mathrm{s}\) and a frequency of \(240 \mathrm{~Hz}\). The amplitude of the standing wave at an antinode is \(0.400 \mathrm{~cm}\). (a) Calculate the amplitude at points on the string a distance of (i) \(40.0 \mathrm{~cm}\) (ii) \(20.0 \mathrm{~cm} ;\) and (iii) \(10.0 \mathrm{~cm}\) from the left end of the string. (b) At each point in part (a), how much time does it take the string to go from its largest upward displacement to its largest downward displacement? (c) Calculate the maximum transverse velocity and the maximum transverse acceleration of the string at each of the points in part (a).

A water wave traveling in a straight line on a lake is described by the equation $$ y(x, t)=(2.75 \mathrm{~cm}) \cos (0.410 \mathrm{rad} / \mathrm{cm} x+6.20 \mathrm{rad} / \mathrm{s} t) $$ where \(y\) is the displacement perpendicular to the undisturbed surface of the lake. (a) How much time does it take for one complete wave pattern to go past a fisherman in a boat at anchor, and what horizontal distance does the wave crest travel in that time? (b) What are the wave number and the number of waves per second that pass the fisherman? (c) How fast does a wave crest travel past the fisherman, and what is the maximum speed of his cork floater as the wave causes it to bob up and down?

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