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The longest pipe found in most medium-size pipe organs is 4.88 m (16 ft) long. What is the frequency of the note corresponding to the fundamental mode if the pipe is (a) open at both ends, (b) open at one end and closed at the other?

Short Answer

Expert verified
(a) 35.14 Hz for open pipe, (b) 17.57 Hz for closed pipe.

Step by step solution

01

Understand the Problem

We need to find the frequency of the sound wave produced by a pipe of length 4.88 meters when it vibrates in its fundamental mode. The problem specifies two conditions: (a) the pipe is open at both ends, and (b) the pipe is open at one end and closed at the other.
02

Use the Formula for Pipe Open at Both Ends

For a pipe open at both ends, the fundamental frequency can be calculated using the formula \( f = \frac{v}{2L} \), where \( v \) is the speed of sound in air (approximately 343 m/s at room temperature) and \( L \) is the length of the pipe. Given that \( L = 4.88 \) m, substitute the values into the formula.
03

Calculate Frequency for Open Pipe

Substituting the values, we have:\[ f = \frac{343}{2 \times 4.88} = \frac{343}{9.76} \approx 35.14 \text{ Hz} \]
04

Use the Formula for Pipe Open at One End

For a pipe open at one end and closed at the other, the fundamental frequency is calculated using the formula \( f = \frac{v}{4L} \). We use the same value for \( v \) and substitute \( L = 4.88 \) m into this formula.
05

Calculate Frequency for Closed Pipe

Substituting the values gives:\[ f = \frac{343}{4 \times 4.88} = \frac{343}{19.52} \approx 17.57 \text{ Hz} \]

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Key Concepts

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

Open and Closed Pipes
In the world of acoustics, pipes play a fascinating role in shaping the sounds we hear. A pipe can either be open at both ends or open at one end and closed at the other. These two variations have significant differences.

**Open Pipes**: When a pipe is open at both ends, it allows air to vibrate freely. The air column inside the pipe uses the entire length to produce sound. This type of pipe supports a fundamental frequency where half a wavelength fits within the pipe. For open pipes, the fundamental frequency is given by the formula \( f = \frac{v}{2L} \), where \( v \) is the speed of sound in air, and \( L \) is the length of the pipe.

**Closed Pipes**: In contrast, a closed pipe is open at one end and closed at the other. This formation presents a different boundary condition where only a quarter of a wavelength fits into the pipe's length for the fundamental frequency. Thus, the formula for the frequency here is \( f = \frac{v}{4L} \). This means closed pipes tend to have a lower pitch than open ones of the same length because they operate at a quarter wavelength.

Understanding these differences helps comprehend why different pipes produce different notes in musical instruments.
Harmonics
Harmonics are integral to understanding how musical notes are formed in pipes. They are basically the overtones or "extra notes" that occur naturally as air vibrates within a pipe.

**Fundamental Frequency**: This is the lowest frequency at which a pipe vibrates. It's called the first harmonic. The other possible frequencies, called higher harmonics, are whole-number multiples of this fundamental frequency.

**Higher Harmonics**: In open pipes, harmonics include all multiples of the fundamental frequency. For example, if the fundamental frequency is 100 Hz, the harmonics would be 200 Hz, 300 Hz, 400 Hz, etc.

In closed pipes, only the odd-numbered harmonics are present. So, if the fundamental is 100 Hz, the harmonics would be 300 Hz, 500 Hz, and so on. This unique characteristic gives closed pipes a distinct sound compared to open pipes. Understanding harmonics is crucial because it is the blend of these frequencies that creates the rich and complex sounds in music.
Wave Speed in Air
The speed of sound, or wave speed in air, is a foundational concept when dealing with sound in pipes. It influences the frequency that we hear.

**Speed Basics**: Sound travels as a wave through the air, and its speed is dependent on the medium. For air at room temperature, the speed is approximately 343 meters per second (m/s).

**Dependence Factors**: The speed of sound can change based on temperature, humidity, and altitude. Warmer air, for example, allows sound to travel faster because the air molecules move more quickly, facilitating quicker transmission of sound waves.

**Practical Application**: When calculating frequencies in pipes, using the correct speed is crucial. Miscalculating the wave speed can lead to an inaccurate determination of the frequency. In our exercise, assuming the wave speed of 343 m/s allows for a precise calculation of the fundamental frequencies for both open and closed pipes.
Understanding the wave speed is essential not only in musical applications but also in various engineering and scientific fields where accurate sound modeling is required.

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Most popular questions from this chapter

The motors that drive airplane propellers are, in some cases, tuned by using beats. The whirring motor produces a sound wave having the same frequency as the propeller. (a) If one single-bladed propeller is turning at 575 rpm and you hear 2.0-Hz beats when you run the second propeller, what are the two possible frequencies (in rpm) of the second propeller? (b) Suppose you increase the speed of the second propeller slightly and find that the beat frequency changes to 2.1 Hz. In part (a), which of the two answers was the correct one for the frequency of the second single-bladed propeller? How do you know?

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