/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 48 This problem represents a possib... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

This problem represents a possible (but not recommended) way to code instantaneous pressures in a sound wave into 16 -bit digital words. Example 17.2 mentions that the pressure amplitude of a \(120-\mathrm{dB}\) sound is \(28.7 \mathrm{N} / \mathrm{m}^{2}\) Let this pressure variation be represented by the digital -code \(65536 .\) Let zero pressure variation be represented on the recording by the digital word \(0 .\) Let other intermediate pressures be represented by digital words of intermediate -size, in direct proportion to the pressure. (a) What digital word would represent the maximum pressure in a \(40 \mathrm{dB}\) -sound? (b) Explain why this scheme works poorly for soft -sounds. (c) Explain how this coding scheme would clip off half of the waveform of any sound, ignoring the actual -shape of the wave and turning it into a string of zeros. By introducing sharp corners into every recorded waveform, this coding scheme would make everything sound like a buzzer or a kazoo.

Short Answer

Expert verified
The digital word representing the pressure of a 40dB sound would be 65 according to this model. This coding scheme is problematic for soft sounds as it would lead to a loss of precision due to the low numbers associated with these sounds. Moreover, this model only captures the absolute magnitude of the sound waves, clipping off the negative halves, which distorts the true nature of the sound waves and introduces a distorted output that can be likened to a buzzy or kazoo-like sound.

Step by step solution

01

Understand Pressure to Decibel Relationship

The ratio of the pressures of two sounds is given by the formula \( \frac{P_{1}}{P_{2}} = 10^{ [(dB_{1}-dB_{2})/20] } \)\n\nWhere \( P_1 \) and \( P_2 \) are the pressures of the two sounds and \( dB_1 \) and \( dB_2 \) their associated decibel levels. The decibel is a logarithmic unit, so this ratio relies on the properties of logarithms.
02

Find the Pressure for a 40dB Sound

Substitute \( dB_1=120 \), \( dB_2=40 \), and \( P_1=28.7 N/m^{2} \) into the formula to find \( P_2 \).\n\nThis gives us \( P_2 = P_1 \times 10^{ [(dB_1-dB_2)/20] } = 28.7 N/m^{2} \times 10^{ [-80/20] } = 0.0287 N/m^{2} \)
03

Assess Corresponding Digital Word for a 40dB Sound's Pressure

Since zero pressure variation is represented by the digital word 0 and the pressure of 28.7N/m² is represented by the digital word 65536, there is a direct proportion between pressure and digital word. Therefore, we can find the digital word that represents the pressure of the 40dB sound, which is 0.0287N/m², by using a simple proportion:\n\n\( \frac{65536}{28.7 N/m^2} = \frac{x}{0.0287 N/m^2} \)\n\nSolving for \(x\), we get \(x = 65536 \times \frac{0.0287 N/m^2}{28.7 N/m^2} = 65 \). So the digital word representing the 40dB sound's pressure should be 65.
04

Explain Model Limitation for Soft Sounds

This model fails to accurately represent soft sounds as the digital words for these sounds would be very small, potentially resulting in a lack of precision in the representation. This would lead to a loss of fidelity in the soft sounds as they would not be represented accurately in the digital format.
05

Explain the Clipping Off of Sound Waveforms

This coding scheme retains only the positive peaks of the sound wave, clipping off the negative halves. This means it is only capable of representing the absolute magnitude of the sound wave. This would result in a misrepresentation of the true nature of the sound wave, which in real life would have both positive (increasing pressure) and negative (decreasing pressure) phases. As such, all waveforms are turned into a string of zeros, essentially producing a distorted sound output, similar to a buzzer or a kazoo.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

Key Concepts

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

Sound Pressure Level
Sound pressure level (SPL) describes the intensity of a sound wave. It's a way to measure how strong a sound is using a logarithmic scale. This helps compare very high pressures, like those from a jet engine, to very low pressures, such as a whisper. SPL is measured in decibels (dB), a unit that expresses the ratio of the sound's pressure to a reference pressure, usually the threshold of hearing at 20 µPa.
Understanding SPL is crucial in digital sound encoding as it helps determine how real-world sounds can be represented correctly in the digital domain. When encoding sound digitally, it's important to preserve the SPL to ensure the sound is accurately reproduced during playback. When converting pressure into digital signals, maintaining the correct SPL ensures media like music or recordings render as they were originally intended to be heard.
  • High SPL indicates loud sounds.
  • Low SPL indicates soft sounds.
  • SPL uses a logarithmic scale to simplify comparing vastly different sound pressures.
Decibel Measurement
Decibels (dB) are a fundamental unit of measurement used in audio systems to gauge sound levels. The formula \( \\frac{P_{1}}{P_{2}} = 10^{\frac{(dB_{1}-dB_{2})}{20}} \) shows the ratio between the pressures of two sounds, reflecting the decibel levels. The use of a logarithmic scale allows us to manage a wide range of pressure values without losing granularity.
The decibel system is effectively employed in audio engineering to manage sound levels, allowing audio equipment to adjust sound dynamics appropriately. Its logarithmic nature means each increase of 10 dB represents a 10-fold increase in perceived loudness.
  • Decibels provide a relative measure of sound pressure.
  • They help in sound design for maintaining aural balance.
  • A 10 dB increase is perceived approximately twice as loud by listeners.
Waveform Distortion
Waveform distortion involves changes in the original shape of a sound wave, leading to a loss of audio fidelity. This can happen when the coding scheme inaccurately captures sound, clipping off parts of the wave, particularly during digital encoding.
Distortion occurs if the digital representation retains only the peaks of the sound wave, not reflecting variations in the sound accurately. This problem is highlighted in simplistic coding schemes where only positive waveform peaks are shown, causing all negative waveform parts to vanish. This could result in audio that sounds unnaturally harsh, like a buzzing noise or a kazoo.
  • Distortion changes audio quality adversely.
  • Accurate waveform capture is crucial for high fidelity.
  • Proper encoding is important to preserve the character of sound.
Quantization Error
Quantization error arises in digital sound encoding when there are discrepancies between the actual continuous sound wave and its digital representation. As the system assigns discrete values to the continuous wave's various pressure points, slight errors can occur.
Inaccurate quantization leads to a mismatch where the digital word may not precisely reflect real-world pressure levels, especially if there is a large gap between steps in the digital encoding (e.g., 16-bit encoding). This can significantly affect lower-level sounds, losing detail in softer audio signals, where small errors become proportionally larger.
  • Quantization error is a mismatch in value assignment.
  • It grows as audio level decreases.
  • Accurate sound encoding minimizes quantization error impact.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

The intensity of a sound wave at a fixed distance from a speaker vibrating at \(1.00 \mathrm{kHz}\) is \(0.600 \mathrm{W} / \mathrm{m}^{2} .\) (a) Determine the intensity if the frequency is increased to \(2.50 \mathrm{kHz}\) while a constant displacement amplitude is maintained. (b) Calculate the intensity if the frequency is reduced to \(0.500 \mathrm{kHz}\) and the displacement amplitude is doubled.

A cowboy stands on horizontal ground between two parallel vertical cliffs. He is not midway between the cliffs. He fires a shot and hears its echoes. The second echo arrives \(1.92 \mathrm{s}\) after the first and \(1.47 \mathrm{s}\) before the third. Consider only the sound traveling parallel to the ground and reflecting from the cliffs. Take the speed of sound as \(340 \mathrm{m} / \mathrm{s}\) (a) What is the distance between the cliffs? (b) What If? If he can hear a fourth echo, how long after the third echo does it arrive?

The sound level at a distance of \(3.00 \mathrm{m}\) from a source is \(120 \mathrm{dB} .\) At what distance will the sound level be (a) \(100 \mathrm{dB}\) and (b) \(10.0 \mathrm{dB} ?\)

As a certain sound wave travels through the air, it produces pressure variations (above and below atmospheric pressure) given by \(\Delta P=1.27 \sin (\pi x-340 \pi t)\) in SI units. Find (a) the amplitude of the pressure variations, (b) the frequency, (c) the wavelength in air, and (d) the speed of the sound wave.

Prove that sound waves propagate with a speed given by Equation \(17.1 .\) Proceed as follows. In Figure \(17.3,\) consider a thin cylindrical layer of air in the cylinder, with face area \(A\) and thickness \(\Delta x\). Draw a free-body diagram of this thin layer. Show that \(\Sigma F_{x}=m a_{x}\) implies that \(-[\partial(\Delta P) / \partial x] A \Delta x=\) \(\rho A \Delta x\left(\partial^{2} s / \partial t^{2}\right) .\) By substituting \(\Delta P=-B(\partial s / \partial x),\) obtain the wave equation for sound, \((B / \rho)\left(\partial^{2} s / \partial x^{2}\right)=\left(\partial^{2} s / \partial t^{2}\right) .\) To a mathematical physicist, this equation demonstrates the existence of sound waves and determines their speed. As a physics student, you must take another step or two. Substitute into the wave equation the trial solution \(s(x, l)=\) \(s_{\max } \cos (k x-\omega t) .\) Show that this function satisfies the wave equation provided that \(\omega / k=\sqrt{B / \rho} .\) This result reveals that sound waves exist provided that they move with the speed \(v=f \lambda=(2 \pi f)(\lambda / 2 \pi)=\omega / k=\sqrt{B / \rho}\)

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.