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Two adjacent nahural frequencies of an organ pipe arc found to be \(550 \mathrm{H}_{2}\) and \(650 \mathrm{~Hz}\). Calculate the fundamenual frequency and length of this pipe. (Use \(v=340 \mathrm{~m} / \mathrm{s}\).) Determine whether the pipe is open at both ends or open at only one end.

Short Answer

Expert verified
The pipe is open at both ends, the fundamental frequency is \(100 Hz\) and the length of the pipe is \(1.7 m\).

Step by step solution

01

Determine the Mode of Vibration

To find the mode of vibration, subtract the lower given frequency from the higher frequency. When subtracted \(650Hz - 550 Hz = 100 Hz\). This difference is actually equivalent to the fundamental frequency or the first harmonic.\n Using this information, we can conclude the pipe is open at both ends because for a pipe open at both ends, the difference between two successive frequencies is always equal to the first harmonic or fundamental frequency.
02

Determine the Fundamental Frequency

As determined in Step 1, the fundamental frequency (first harmonic) is \(100 Hz\).
03

Determine the Length of the Pipe

To find the length of the pipe, we use the formula for the fundamental frequency of a pipe open at both ends: \[f1 = v/(2L)\] Solving for \(L\), we get: \[L = v/(2f1)\] Substituting the given values, we find: \(L = (340 m/s) / (2 * 100 Hz) = 1.7 m\]

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Key Concepts

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

Organ Pipe Resonances
Organ pipe resonances are a fascinating application of the principles of acoustics that produce the rich and varied sounds of organ music. These resonances occur due to the standing waves set up within the pipes when they are played. Depending on whether an organ pipe is open at both ends or just one, different patterns of resonances, or 'harmonics,' can be produced.

For an open organ pipe, resonances occur at frequencies that are multiples of the fundamental frequency—the lowest frequency at which the pipe resonates. Closed pipes, on the other hand, only resonate at odd multiples of the fundamental frequency. This principle helps musicians and organ builders design pipes that produce desired pitches and tones.
Acoustics
Acoustics, the study of sound, helps us understand how organ pipes and other musical instruments work. The fundamental elements of acoustics include frequency, amplitude, and wavelength, which determine the pitch, loudness, and harmonic content of the sound respectively. Sound waves travel through different mediums at different speeds; in air, they travel at approximately 340 meters per second. When these waves encounter objects, they can be reflected, absorbed, or transmitted, which greatly affects the sound's volume and quality, crucial for the design of musical instruments and concert halls.
Harmonics
Harmonics are integral to the sound of musical instruments, including organs. They are the integer multiples of the fundamental frequency and contribute to the timbre—or color—of sound. In our exercise, harmonics help determine the type of organ pipe based on their natural frequencies. When analyzing sound, understanding harmonics is essential to uncovering the character and quality of the note played.

For example, when an organist plays a key, a complex wave composed of the fundamental frequency and its harmonics is produced, resulting in the unique sound of the instrument. A fuller and richer tone usually contains a large number of harmonics.
Wavelength of Sound
The wavelength of a sound is the physical distance over which the wave's shape repeats. It is inversely proportional to the frequency of the sound, with higher frequencies having shorter wavelengths. Mathematically, it can be expressed with the equation \( \text{Wavelength} = \frac{v}{f} \), where \( v \) is the speed of sound in the medium, and \( f \) is the frequency of the sound.

In terms of musical instruments, such as an organ pipe, the length of the pipe is related to the wavelength of its fundamental frequency. Longer pipes create longer wavelengths and thus lower pitches. This is why bass pipes in organs are so much larger than the pipes used for higher notes.

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Most popular questions from this chapter

The human ear canal is about \(2.8 \mathrm{~cm}\) long. If it is regarded as a tube that is open at one end and closed at the eardrum, what is the fundamental frequency around which we would expect hearing to be most sensitive? Take the speed of sound to he \(340 \mathrm{~m} / \mathrm{s}\).

At rest, a car's horn sounds the note A \((440 \mathrm{H} z)\). The horn is sounded while the car is moving down the strect. A bicyclist meving in the same direction with one-third the car's speed hears a frequency of \(415 \mathrm{~Hz}\). What is the speed of the car? Is the cyclist ahead of or behind the car?

Show that the difference in decibel levels \(\beta_{1}\) and \(\beta_{2}\) of a sound source is related to the ratio of its distances \(r_{1}\) and \(r_{2}\) from the receivers by the formula $$ \beta_{2}-\beta_{1}=20 \log \left(\frac{r_{1}}{r_{2}}\right) $$

An outside loudspeaker (considered a small source) emits sound waves with a power output of \(100 \mathrm{~W}\). (a) Find the intensity \(10.0 \mathrm{~m}\) from the source, (b) Find the intensity level in recibels at that distance. (c) At what distance would you experience the sound at the threshold of pain, \(120 \mathrm{~dB}\) ?

\(A\) quartz watch contains a crystal oscillator in the form of a block of quartz that vibrates by contracting and expanding. Two opposite faces of the block, \(7.05 \mathrm{~mm}\) apart, are antinodes, moving alternately toward and away from each other. The plane halfway between these two faces is a node of the vibration. The speed of sound in quartz. is \(3.70 \mathrm{~km} / \mathrm{s}\). Find the frequency of the vibration. An oscillating electric voltage accompanies the mechanical

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