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An organ is in tune at \({\bf{22}}{\bf{.}}{{\bf{0}}^{\bf{o}}}{\bf{C}}\). By what percent will the frequency be off at \({\bf{1}}{{\bf{1}}^{\bf{o}}}{\bf{C}}\)?

Short Answer

Expert verified

The percentage frequency be off at \(11{\rm{^\circ C}}\) is \( - 1.917\% \).

Step by step solution

01

Relationship between the speed of sound, frequency, and temperature.

The speed of sound is directly related to the change in the temperature, and this change in temperature is directly related to the change in frequency.\(v \propto T \propto f\).

02

Calculation of change in frequency

The expression for the frequency at\(22{\rm{^\circ C}}\)is given as,

\({f_{22{\rm{^\circ C}}}} = \frac{{{v_{22{\rm{^\circ C}}}}}}{\lambda }\)

Here,\({v_{22^\circ C}}\)is the speed of the sound at\(22{\rm{^\circ C}}\)and\(\lambda \)is the resonant wavelength inside the pipe.

The expression for the frequency at\(11{\rm{^\circ C}}\)is given as,

\({f_{{\rm{11^\circ C}}}} = \frac{{{v_{{\rm{11^\circ C}}}}}}{\lambda }\)

Here,\({v_{11^\circ C}}\)is the speed of the sound at\(11{\rm{^\circ C}}\).

The expression for the change in frequency is given as,

\(\Delta f = {f_{11{\rm{^\circ C}}}} - {f_{{\rm{22^\circ C}}}}\)

Substitute the values in the above equation,

\(\begin{array}{c}\Delta f = \frac{{{v_{{\rm{11^\circ C}}}}}}{\lambda } - \frac{{{v_{{\rm{22^\circ C}}}}}}{\lambda }\\ = \frac{{{v_{{\rm{11^\circ C}}}} - {v_{{\rm{22^\circ C}}}}}}{\lambda }\end{array}\)

03

Calculation of the percentage change in the frequency.

The ratio of change in frequency to the original frequency is given as,

\(\begin{array}{c}\frac{{\Delta f}}{{{f_{22^\circ {\rm{C}}}}}} = \frac{{\frac{{{v_{{\rm{11^\circ C}}}} - {v_{{\rm{22^\circ C}}}}}}{\lambda }}}{{\frac{{{v_{{\rm{22^\circ C}}}}}}{\lambda }}}\\ = \frac{{{v_{{\rm{11^\circ C}}}}}}{{{v_{{\rm{22^\circ C}}}}}} - 1\end{array}\)…… (i)

The speed of sound at\(22{\rm{^\circ C}}\)can be written as,

\({v_{22{\rm{^\circ C}}}} = 331 + 0.6{T_{22{\rm{^\circ C}}}}\)

The speed of sound at\(11{\rm{^\circ C}}\)can be written as,

\({v_{{\rm{11^\circ C}}}} = 331 + 0.6{T_{{\rm{11^\circ C}}}}\)

Substitute the values in equation (i),

\(\frac{{\Delta f}}{{{f_{22^\circ {\rm{C}}}}}} = \frac{{331 + 0.6{T_{{\rm{11^\circ C}}}}}}{{331 + 0.6{T_{{\rm{22^\circ C}}}}}} - 1\)

The percentage difference is,

\(\begin{array}{c}\frac{{\Delta f}}{{{f_{22^\circ {\rm{C}}}}}} = \left( {\frac{{331 + 0.6\left( {11{\rm{^\circ C}}} \right)}}{{331 + 0.6\left( {{\rm{22^\circ C}}} \right)}} - 1} \right) \times 100\% \\ = - 0.01917 \times 100\% \\ = - 1.917\% \end{array}\)

Thus, the percentage frequency be off at \(11{\rm{^\circ C}}\) is \( - 1.917\% \).

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Most popular questions from this chapter

(II) In one of the original Doppler experiments, a tuba was played at a frequency of 75 Hz on a moving flat train car, and a second identical tuba played the same tone while at rest in the railway station. What beat frequency was heard in the station if the train car approached the station at a speed of 14.0 m/s?

Question: (II) An unfingered guitar string is 0.68 m long and is tuned to play E above middle C (330 Hz). (a) How far from the end of this string must a fret (and your finger) be placed to play A above middle C (440 Hz)? (b) What is the wavelength on the string of this 440-Hz wave? (c) What are the frequency and wavelength of the sound wave produced in air at 22°C by this fingered string?

A person, with his ear to the ground, sees a huge stone strike the concrete pavement. A moment later two sounds are heard from the impact: one travels in the air and the other in the concrete, and they are 0.80 s apart. How far away did the impact occur? See Table 12-1.

Question: (II) Two violin strings are tuned to the same frequency, 294 Hz. The tension in one string is then decreased by 2.5%. What will be the beat frequency heard when the two strings are played together? (Hint: Recall Eq. 11–13.)

(III) Two loudspeakers are placed 3.00 m apart, as shown in Fig. 12–37. They emit 474-Hz sounds, in phase. A microphone is placed 3.20 m distant from a point midway between the two speakers, where an intensity maximum is recorded. (a) How far must the microphone be moved to the right to find the first intensity minimum? (b) Suppose the speakers are reconnected so that the 474-Hz sounds they emit are exactly out of phase. At what positions are the intensity maximum and minimum now?

Figure 12-37

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