Guitar String. One of the \(63.5\;{\rm{cm}}\)-long strings of an ordinary guitar is tuned to produce the note \({B_3}\) (frequency \(245\;{\rm{Hz}}\)) when vibrating in its fundamental mode. (a) Find the speed of transverse waves on this string.

(b) If the tension in this string is increased by \(1.0\% \), what will be the new fundamental frequency of the string?

(c) If the speed of sound in the surrounding air is \(344\;{{\rm{m}} \mathord{\left/ {\vphantom {{\rm{m}} {\rm{s}}}} \right. \\} {\rm{s}}}\), find the frequency and wavelength of the sound wave produced in the air by the vibration of the \({B_3}\) string. How do these compare to the frequency and wavelength of the standing wave on the string?

Short Answer

Expert verified

(a) The speed of transverse waves is, \(311.15\;{{\rm{m}} \mathord{\left/ {\vphantom {{\rm{m}} {\rm{s}}}} \right. \\} {\rm{s}}}\).

Step by step solution

01

Identification of the given data

The given data can be listed below as,

  • The length of the string is, \(L = 63.5\;{\rm{cm}} = 63.5 \times {10^{ - 2}}\;{\rm{m}}\).
  • The fundamental frequency is, \({f_1} = 245\;{\rm{Hz}}\).
02

Significance of the speed of transverse waves

A wave's velocity is its rate of movement. By using the formula wave speed is equal to the product of frequency and wavelength, wave speed is correlated with wavelength, frequency, and period. Visible light, an electromagnetic wave, travels at a speed that is most frequently employed.

03

Determination of the speed of transverse waves

The relation between fundamental frequency, velocity and length of string is expressed as,

\({f_1} = \frac{v}{{2L}}\) …(1)

Here \({f_1}\) is the fundamental frequency, \(v\) is the velocity and \(L\) is the length of string.

Substitute \(245\;{\rm{Hz}}\) for \({f_1}\) and \(63.5 \times {10^{ - 2}}\;{\rm{m}}\) for \(L\) in the equation (1).

\(\begin{array}{c}245\;{\rm{Hz}} = \frac{v}{{2 \times 63.5 \times {{10}^{ - 2}}\;{\rm{m}}}}\\v = \left( {245\;{\rm{Hz}}} \right) \times \left( {2 \times 63.5 \times {{10}^{ - 2}}\;{\rm{m}}} \right)\\v = 311.15\;{{\rm{m}} \mathord{\left/ {\vphantom {{\rm{m}} {\rm{s}}}} \right. \\}{\rm{s}}}\end{array}\)

Hence the speed of transverse waves is, \(311.15\;{{\rm{m}} \mathord{\left/ {\vphantom {{\rm{m}} {\rm{s}}}} \right. \\} {\rm{s}}}\).

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Most popular questions from this chapter

A heavy rope 6.00 m long and weighing 29.4 N is attached at one end to a ceiling and hangs vertically. A 0.500-kg mass is suspended from the lower end of the rope. What is the speed of transverse waves on the rope at the (a) bottom of the rope, (b) middle of the rope, and (c) top of the rope? (d) Is the tension in the middle of the rope the average of the tensions at the top and bottom of the rope? Is the wave speed at the middle of the rope the average of the wave speeds at the top and bottom? Explain.

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