Chapter 2 Flashcards

1
Q

Motions of Vibrating Air Molecules

A

Sound can be defined as the propagation of a pressure wave–sound wave–in space and time
Sound must be propagated through a medium
The medium is composed of molecules that are compressible (degree of compressibility depends on the medium)
Force displaces molecules of the medium from “rest positions” and moves them closer to nearby molecules and results in a “bunching up” of molecules

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2
Q

All sound-conducting media have

A

ll sound-conducting media have elasticity & mass
Elastic objects oppose displacement
Massive objects oppose being accelerated and decelerated
Generally, the medium of interest for speech is air
Molecules at rest are still in motion–Brownian Motion
Average spacing between molecules is roughly equivalent

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3
Q

When a molecule is subjected to a force

A

When a molecule is subjected to a force, it moves away from its rest position and in the direction of the force
As it moves farther from its rest position, it opposes increasing displacement by generating an increasing recoil force which is exerted in the direction of the rest position
This displacement continues as molecules bump into neighboring molecules and this is how the sound wave is propagated

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4
Q

Pressure can be defined

A

Pressure can be defined as the force exerted over a unit area (P=F/A)
Proportional to the density of air

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5
Q

When air molecules are more densely packed in some unit volume

A

When air molecules are more densely packed in some unit volume, they collide with each other more frequently and generate more force and pressure within the volume.
Conversely, when air molecules are less densely packed, the collisions are less frequent and the pressures are relatively lower
The density of air at rest is the same at any spatial location–atmospheric pressure
Atmospheric pressure serves as a reference for positive & negative pressure

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6
Q

compression or condensation

A

High-density and high-pressure areas are called areas of compression or condensation

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7
Q

rarefaction

A

Low-density and low-pressure areas are called areas of rarefaction

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8
Q

Pressure Waves Propagate Through Space

A

Individual molecules don’t propagate through space
Molecules move around a rest position, movement results from inherent elastic and inertial forces
The pressure wave moves across space as a sequence of compressions and rarefaction areas
The air molecules move back and forth which alternately bunches them up and spreads the apart
Sound is a longitudinal wave
When a pressure wave moves away from the source of the sound waves, the alternating regions of high and low pressures the same direction as the force

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9
Q

Measuring Variation of a Pressure Wave in Time & Space

A

There are specific measures of the temporal (time) and spatial (space) variation of pressure waves
A waveform shows a magnitude (e.g., displacement, pressure, etc.) as a continuous function of time
A waveform shows one complete cycle of motion
Period (T) is the time taken to complete one full cycle of motion
Frequency (f) is the number of cycles of vibrations completed in one second
Hertz (Hz)–cycles per second
T=1/f
Period and Frequency have a nonlinear relationship

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10
Q

Wavelength

A

Wavelength–distance covered by a high-pressure region and its succeeding low-pressure region (or vice versa)
It is the measurement of spatial variation of a wave
Symbolized by greek letter lambda λ

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11
Q

Spatial Measures

A

Wavelength–distance covered by a high-pressure region and its succeeding low-pressure region (or vice versa)
It is the measurement of spatial variation of a wave
Symbolized by greek letter lambda λ
Has an inverse relationship to frequency
The higher the frequency, the shorter the wavelength

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12
Q

When sound waves encounter an object along their path

A

When sound waves encounter an object along their path, straight-line propagation may change
Frequencies with very long wavelengths generally may bend around objects in their path
Frequencies with very short wavelengths may strike the object and cause pressure variation to reflect off the object
The pressure reflections interact with the original pressure wave as well as with the multiple reflections
The relationship between wavelength and objects within the path of a pressure wave is related to their respective magnitudes

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13
Q

The motions of air molecules can produce pressure waves

A

The motions of air molecules can produce pressure waves, which are the basis of sound
Pressure waves vary across space and time
Can be described and measured in mathematical terms
The simple motions and resulting pressure waves discussed previously were sinusoidal motions and waves
Simplest form of vibration
Complex vibrations can be broken down into component individual sinusoids

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14
Q

Sinusoidal Motion

A

Simple Harmonic Motion
Linear projection of uniform circular speed (UCS)

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15
Q

Frequency:

A

number of full cycles occurring in a one second interval (f)

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16
Q

Amplitude:

A

: displacement of an air molecule from the rest position (A)

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17
Q

Phase:

A

position of the sinusoidal motion relative to some arbitrary reference position (φ)

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18
Q

Sinusoidal Motion Summary

A

A sine wave is a waveform that results from the linear projection of UCS
A sine wave is periodic
A sine wave involves only a single frequency
Simplest type of acoustic event
Described by a simple formula including the parameters of period, amplitude, and phase

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19
Q

Complex Acoustic Events

A

Acoustic event contains more than one frequency
Two types of complex events
Periodic: waveform pattern repeats over time
Aperiodic: no repeating pattern can be identified

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20
Q

Periodic

A

: waveform pattern repeats over time

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21
Q

Aperiodic

A

no repeating pattern can be identified

22
Q

Waveform

A

shows an acoustic event in the time domain
Shows frequency, period, and amplitude but not individual harmonics

23
Q

Spectrum

A

shows an acoustic event in the frequency domain
Shows harmonic content of a sound but does not show changes over time

24
Q

Complex Periodic Event

A

Has a waveform that repeats its pattern over time
Composed of harmonically related frequency components
Fundamental frequency–lowest component frequency in a complex periodic sound
Waveform shows an acoustic event in the time domain
Shows frequency, period, and amplitude but not individual harmonics
Spectrum shows an acoustic event in the frequency domain
Shows harmonic content of a sound but does not show changes over time

25
Q

Sum of Individual Sinusoids at the Harmonic Frequencies

A

Complex periodic waveforms have spectra with multiple, harmonically related frequencies
Energy at these frequencies is discrete
Spectral representations show a snapshot of component sinusoids of a complex acoustic event across an interval of time
Spectrum shows the acoustic event with individual frequency components “pulled apart” and displayed with their relative amplitudes
Requires Fourier analysis

26
Q

Superposition principle:

A

Superposition principle: when waveforms of different sinusoidal frequencies are viewed on the same time scale, at any point in time the amplitude of the complex waveform is the sum of the amplitudes of each of the component sinusoids, at that point in time
It is as if the sinusoids are ‘superimposed’ on each other to create a complex waveform whose shape over time reflects the amplitude contributions of each component sinusoid

27
Q

Beats

A

Perceptual result of two similar sinusoids slowly and systematically going in and out of phase

28
Q

When two or more sinusoids are related to each other

A

When two or more sinusoids are related to each other by a whole number multiple, they are said to be in harmonic relationship
When individual sinusoidal components of an acoustic event are harmonically related, the complex event will be periodic

29
Q

Complex Aperiodic Events

A

Have waveforms in which no repetitive pattern can be discerned
Frequency components are not harmonically related
White noise–complex aperiodic acoustic event that contains energy at all frequencies

30
Q

Complex Acoustic Events: Summary

A

Complex acoustic events are composed of more than one frequency
May be periodic or aperiodic
Periodic events have a repetitive waveform pattern and a fundamental frequency
Aperiodic events do not have a fundamental frequency because the waveform is nonrepetitive
Can be displayed in either time domain (waveform) or frequency domain (spectrum)

31
Q

Resonance

A

The phenomenon whereby an object vibrates with maximum energy at a particular frequency or range of frequencies
“Natural frequency” is sometimes used synonymously with the term “resonance”
Doesn’t mean the object vibrates at only one frequency
Rather, there is a frequency that naturally produces a vibration of greatest amplitude

32
Q

Mass & Elasticity Contributions in resonance

A

The relative values of mass (M) and elasticity (K) determine the frequency of vibration of the spring-mass model
Mass of an object is defined as its weight divided by the value of acceleration due to gravity
Objects with mass have inertia–opposition to being accelerated and decelerated
This property explains why when an air molecule recoils from a stretched or compressed position back toward the rest position, it doesn’t stop at the rest position.
Elasticity, amount of force needed to displace an object, is measured in terms of Stiffness(K)
K=force/meters
Stiffer objects require greater force to displace them

33
Q

Effects of Mass and Stiffness on a Resonant System: Summary

A

A decrease in resonant frequency can be accomplished either by a decrease in stiffness or an increase in mass
Increase in resonant frequency can be accomplished either by an increase in stiffness or a decrease in mass
In complicated resonant systems, both stiffness and mass vary independently and their ratio determines the resonant/natural frequency of the system

34
Q

Acoustic Resonance: Helmholtz Resonators

A

Named in honor of a german scientist, Hermann von Helmholtz
Resonator consists of: length l, circular opening with radius a, and a bowl with radius R

35
Q

Neck of Helmholtz Resonator

A

The neck of the resonator contains a plug of air that behaves like a mass when a force is applied to it
When a force is applied to the plug of air, or acoustic mass (Ma), it offers opposition to being accelerated and, once set in motion, opposition to being decelerated
Behaves like the mass-spring models that were previously discussed
Increase in Ma decreases the resonant frequency (fr) of a Helmholtz resonator
Longer neck
Decrease size of neck opening

36
Q

Bowl of a Helmholtz Resonator

A

When a force is applied to the air in the bowl, molecules are compressed or expanded (like the spring in the spring-mass model)
When the air is compressed, the molecules exert a recoil force to “spring back” to their rest positions
The recoil forces are expressed as pressures above or below atmospheric pressure (Patm)
Compressions create positive pressures
Expansions create negative pressures
Acoustic compliance (Ca) denotes stiffness properties of the volume of air within a resonator bowl
Compliance is the inverse of stiffness–stiffer volume of air is less compliant
Ca can be varied by changing the size of the bowl
An increase in Ca (i.e., a decrease in stiffness) decreases the fr in a Helmholtz resonator

37
Q

Acoustic Resonance: Tube Resonators

A

Tubes are a class of resonators with substantial relevance to speech acoustics
Different considerations for tubes that are open at both ends and tubes that are closed at one end

38
Q

Tubes open at both ends

A

Pressure at the two open ends is Patm
Therefore, there must be frequencies whose wavelengths distribute pressure over space in a way that has Patm at both ends of the tube

39
Q

Standing Waves

A

Occurs when vibrating air molecules within a tube produce the same pressure variations at that same location within the tube
These pressures reinforce each other and build up to their maximum value
Standing waves occur at resonant frequencies
Tubes open at both ends have multiple resonant frequencies because multiple frequencies have wavelengths that match the requirement of Patm at the end

40
Q

Calculating the Resonant Frequency of an Open Tube

A

IF the length of a tube is known, one must double it to get another wavelength and frequency that produces the desired pressure match at the ends of the tube
Half-wavelength rule
fr = n*c/2l
Fr = resonant frequency
C = constant, speed of sound in air
l = length of the tube
n = multiplier that can be any integer

41
Q

Tube with One End Closed

A

Pressure at the open end is Patm and pressure at the closed end is maximum (greatest pressure along the wavelength)

42
Q

Calculating Resonant Freq of a Tube with One Closed End

A

Quarter-wavelength rule
One-quarter of a wavelength “fits” the pressure requirements for resonance of the tube
fr = (2n - 1) * c/4l
fr = resonant frequency
C = constant, speed of sound in air
l = length of the tube
n = multiplier that can be any integer

43
Q

Resonance in Tubes: Summary

A

Tubes resonate at multiple frequencies because wavelengths of multiple frequencies have pressure distributions for resonance that meet the pressure requirements at the ends of the tube

44
Q

Resonance Curves, Damping & Bandwidth

A

Natural vibratory phenomena are characterized by loss of energy over time which reduces the amplitude of vibration over time, and eventually terminates the vibration
Damping is the term to describe energy loss in vibratory systems
Lightly damped systems have minimal energy loss
Heavily damped systems have substantial energy loss

45
Q

Four Factors that Cause Damping in Vibratory Systems

A

Friction: produced when objects rub against each other or other structures, producing heat
Absorption: vibrating object transfers some of its energy to another structure
Radiation: when air is vibrating within a resonator, some of the sound energy escapes or radiates from the tube and is lost
Gravity: force that attracts any mass to earth, opposes the forces inherent to vibration (e.g., recoil & inertia).
Not a major consideration in acoustic vibratory systems. Can be observed in degradation of pendulum motion

46
Q

Friction:

A

Friction: produced when objects rub against each other or other structures, producing heat

47
Q

Absorption:

A

Absorption: vibrating object transfers some of its energy to another structure

48
Q

Radiation:

A

when air is vibrating within a resonator, some of the sound energy escapes or radiates from the tube and is lost

49
Q

Gravity:

A

force that attracts any mass to earth, opposes the forces inherent to vibration (e.g., recoil & inertia).
Not a major consideration in acoustic vibratory systems. Can be observed in degradation of pendulum motion

50
Q

Bandwidth

A

Range of frequencies between the two 3-db-down points on either side of peak energy
A perfectly tuned resonator has energy at a single frequency (and spectrum would reflect a single vertical line at a given frequency)
Damping factors change this tuning and produce energy at frequencies other than the natural frequency
The frequency-domain index of this tuning is called the bandwidth of the resonator

51
Q

Shaping of a Source by the resonator characteristics

A

A resonator is a filter to the sound source
A filter passes certain inputs through and rejects others
Resonant freqs are passed through and others are rejected to varying degrees

52
Q

Resonance, Damping, Bandwidth, Filters: Summary

A

Vibratory patterns of air in resonators are characterized by resonant frequency and energy loss factors that determine the shape of the curve around the peak
Energy loss factors can be described in the time or frequency domain
Greater energy loss is associated with
More rapid decay of vibratory amplitude over time
Wider bandwidths
Resonators filter inputs and produce an output that reflects the combination of the input and resonator characteristics