Question: A dramatic demonstration, called “singing rods,” involves a long, slender aluminum rod held in the hand near the rod’s midpoint. The rod is stroked with the other hand. With a little practice, the rod can be made to “sing,” or emit a clear, loud, ringing sound. For an \({\bf{80}}\)-cm-long rod, (a) what is the fundamental frequency of the sound? (b) What is its wavelength in the rod, and (c) what is the traveling wavelength of the sound in air at\({\bf{2}}{{\bf{0}}^{\bf{o}}}{\bf{C}}\)?

Short Answer

Expert verified

(a) The fundamental frequency of the sound is\(3187.5\,{\rm{Hz}}\).

(b) The wavelength of the rod is\({\rm{1}}{\rm{.6}}\,{\rm{m}}\).

(c) The traveling wavelength of the sound in air is\(0.1076\,{\rm{m}}\).

Step by step solution

01

Concept

For an open tube open tube with length \(l\) , the fundamental frequency is \(f = \frac{v}{{2l}}\). Here, \(v = 5000\;{\rm{m/s}}\)is the speed of sound in the metal.

02

Given Data

The length of the room is \(l = 80\;{\rm{cm}} = 80\;{\rm{cm}} \times \frac{{1\;{\rm{m}}}}{{100\;{\rm{cm}}}} = 0.80\;{\rm{m}}\).

03

Calculation

Part (a)

The frequency of the fundamental tone for the length is,

\(\begin{array}{c}f = \frac{v}{{2l}}\\f = \frac{{5000\,{\rm{m/s}}}}{{2\left( {0.80\,{\rm{m}}} \right)}}\\f \approx 3187.5\,{\rm{Hz}}\end{array}\)

Hence the fundamental frequency is \(3187.5\,{\rm{Hz}}\).

Part (b)

The wavelength of sound in the rod is two times its length which is,

\(\begin{array}{c}\lambda = 2 \times 0.8\;{\rm{m}}\\ = {\rm{1}}{\rm{.6}}\,{\rm{m}}\end{array}\)

Hence, the wavelength is \({\rm{1}}{\rm{.6}}\,{\rm{m}}\).

Part (c)

The frequency and speed of sound in air determine the wavelength of the sound in air.

\(\begin{array}{c}\lambda ' = \frac{v}{f}\\ = \frac{{343\,{\rm{m/s}}}}{{3187.5\,{\rm{Hz}}}}\\ \approx 0.1076\,{\rm{m}}\end{array}\)

Hence, the traveling wavelength of the sound in air is \(0.1076\,{\rm{m}}\).

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Most popular questions from this chapter

A guitar string vibrates at a frequency of 330 Hz with a wavelength 1.40 m. The frequency and wavelength of this sound in air (20°C) as it reaches our ears is

(a) same frequency, same wavelength.

(b) higher frequency, same wavelength.

(c) lower frequency, same wavelength.

(d) same frequency, longer wavelength.

(e) same frequency, shorter wavelength.

If a wind is blowing, will this alter the frequency of the sound heard by a person at rest with respect to the source? Is the wavelength or velocity changed?

Question: (III) The human ear canal is approximately 2.5 cm long. It is open to the outside and is closed at the other end by the eardrum. Estimate the frequencies (in the audible range) of the standing waves in the ear canal. What is the relationship of your answer to the information in the graph of Fig. 12–6?

Figure 12–6

Question: (I) A piano tuner hears one beat every 2.0 s when trying to adjust two strings, one of which is sounding 350 Hz. How far off in frequency is the other string?

Question: In audio and communications systems, the gain, \(\beta \) in decibals is defined for an amplifer as,

\(\beta = {\bf{10log}}\left( {\frac{{{P_{{\bf{out}}}}}}{{{P_{{\bf{in}}}}}}} \right)\)

Where \({P_{{\bf{in}}}}\) is the power input to the system and \({P_{{\bf{out}}}}\) is the power output. (a) A particular amplifer puts out 135 W of power for and input of 1.0 mW. What is its gain in dB? (b) if a signal to noise ratio of 93 dB is specified, what is the noise power if the output signal is 10 W?

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