Acoustics Review Flashcards

1
Q

Importance of understanding acoustics

A

Reading Audiograms
Understanding Hearing loss
Environmental Acoustics

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2
Q

What is sound?

A

An object makes a sound by
vibrating
The vibrations pass through air
making air molecules vibrate
When the sound pressure waves
reach the ear, hearing may take
place

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3
Q

Physical Acoustics:

A

Propagation of pressure waves through an elastic medium, without permanent
displacement of the particles
Three prerequisites:
◦ Source of energy (eg a force)
◦ Vibrating object
◦ Medium of transmission
A receiver of these prerequisites is optional!

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4
Q

Characteristics of Sound

A

Mass
◦ form of matter capable of vibratory
motion – air molecules

Inertia
◦ tendency to resist change in motion

Elasticity
◦ Restorative property of an object
Simple Harmonic Motion
◦ Compressions and rarefaction
5
6

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5
Q

Simple Harmonic Motion

A

Pure tone
◦ A sound source sets air molecules into vibration.
◦ Air molecules bunch together (compression) and then spread out (rarefaction) at
a steady rate.
◦ Elasticity restores the displaced air molecules to its original resting place
◦ Inertia causes the air molecules to swing past the rest position when returning to
their original state.
◦ This chain reaction of air disturbances create pressure waves that reach our ear
and vibrates the tympanic membrane which transfers the sound to the brain.

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6
Q

Properties of sound

A

Frequency
◦Period
◦Wavelength
Phase
Intensity
(Amplitude)

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7
Q

Frequency
Range of human hearing HZ?

A

of cycles completed in 1 sec
Unit of measurement: Hertz (Hz)
Perceptual correlate: pitch
Human range of hearing: 20 – 20,000 Hz

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8
Q

Wavelength (λ)

A

Distance sound wave travels in
one cycle of vibration
Length of the wave
λ = v/f (v=1130 ft/sec or
340m/sec)
Inverse relationship between f & λ

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9
Q

Wavelength (λ) and Distance
Low vs high frequency

A

Wavelength = velocity/frequency
λ250Hz =1130ft/s/ 250Hz = 4.52 ft
λ8000Hz = 1130ft/s / 8000Hz = .14ft or 1.68 inches
Low frequency sounds have longer wavelengths
that refract or bend more easily around objects
than high frequencies.

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10
Q

Phase

A

Position in time of the displacement
of the air molecules during simple
harmonic motion (how cycles relate
to each other)
Unit of Measurement: Degrees
Standard is 0 degrees

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11
Q

Resonance and frequency

A

All physical objects, if disturbed by another object will begin to
vibrate.
All objects possess a natural resonant frequency
Resonant frequency – frequency rate at which an object will
vibrate with the least amount of externally applied energy,
depending on its specific density and stiffness (elasticity)
For example, a tuning fork with a specific intensity/stiffness will
vibrate at a specific frequency when struck.

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12
Q

Resonance and speech and hearing

A

◦Fundamental frequency of the vocal cords determines the
pitch of the speaker’s voice
◦Length and shape of the vocal tract and articulators provide
clues regarding the identity of the specific sound (formant
frequencies)
◦Length and shape of external auditory meatus resonate at
high frequencies and enhances speech understanding

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13
Q

Frequency and sound localization

A

Diffracton - Sound bends around a barrier
Reflection - Sound bounces off of a barrier
Head Shadow Effect
◦ Low frequencies bend around the head. This creates a phase or time
difference at the opposite ear.
◦ High frequency sounds will not wrap around the head as readily. This
creates a lowering of sound levels at the opposite ear.
Sound localization is dependent on the ear picking up these
phase (time) and intensity cues.

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14
Q

Intensity

A

Intensity is force over unit area
Amplitude of the displacement
Unit of Measurement: decibel (dB)
Perceptual correlate: loudness
Normal human ear can
hear from about 0dB – 140 dB SPL

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15
Q

Micropascals (μPa)

A

Sound waves travel through air and create pressure
waves
Pressure is force / area (Relates to amplitude of the pure
tone)
The greater the change in pressure, the greater the
intensity of sound.
The unit of measurement of air pressure change that we
hear is micropascal (μPa)
Micropascal (μPa) is an absolute unit for measuring
sound pressure

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16
Q

Micropascals and Decibels

A

20 μPa
◦ pressure level of a sound that is just barely audible
◦ Used as a reference value.
200,000,000 μPa
◦ Pressure level of a sound that is painful without shattering the
eardrum
The difference between the softest audible sound and the
loudest tolerable sound represents a huuuge range of
hearing.
The decibel is used to compress this large range of hearing into
more manageable increments.

17
Q

The Decibel

A

Decibel is a unit for expressing
the logarithmic ratio between 2
sound pressures

18
Q

Logarithmic Scale

A

Logarithms (logs) compresses large numbers used in a
linear scale into a much smaller range.
1,000,000 = 10 X 10 X 10 X 10 X 10 X 10
6 multiplications of ten can also be written as 1,000,000
= 10 6
The exponent 6 is the value of the logarithm for base “10”
◦Log 10 (1,000,000) = 6

19
Q

The Decibel and Logarithmic Scale

A

The decibel uses a logarithmic scale to compare the ratio of
intensities of two acoustic sounds
The logarithm of a measured pressure is compared to a reference pressure
It is therefore nonlinear
◦ 10 dB is 10x as loud
◦ 20 dB is 100x as loud
◦ 30 dB is 1000x as loud

20
Q

Decibel Hearing level (dBHL)

A

An audiogram measures
hearing in dB HL
Why do we switch from dB
SPL to dB HL when
measuring a person’s
threshold of hearing?

21
Q

Decibel Hearing level (dBHL)

A

The human ear does not hear
equally well at all frequencies.
Human ear hears best at mid-
frequencies
The human ear requires more
intensity (SPL) to hear low &
very high frequencies

22
Q

SPL, HL and Audiometric Zero

A

The curved SPL scale is normalized. It becomes a flat, straight line at 0 dB HL.
Audiometric 0 (0dB HL represents the amount of sound pressure required by the average young adult to
barely hear a particular frequency.

23
Q

Hearing level (HL)

A

Hearing tests measure a person’s hearing to the hearing of the average young
adults hearing
Each frequency has a different dB SPL threshold level.
Converting dB SPL to dB HL creates the same ‘audiometric 0’ reference for all
frequencies.
The audiometer is calibrated so that 0 dB HL presents a different dB SPL at
each frequency.
Thus, reference SPL values are “built into” the dB HL (hearing level) scale on
the audiogram

24
Q

Clinical audiogram (dBHL)

A

▪Degree of hearing loss is easily
determined using the dB HL reference.
▪The curved dB SPL scale becomes a flat,
straight line (audiometric 0)
▪Degree of hearing loss is determined by
amount of deviation from audiometric 0.
▪Recall, that 0dBHL (Hearing level) uses a
different db SPL reference level for each
test frequency

25
Q

Sensation level (SL)

A

dBSL
Reference is the subject’s threshold level
How much above the person’s threshold is the signal presented
Ex: Threshold is 20 dB HL
Signal is 50 dB HL
The signal is presented at ___ dB SL
49
50

26
Q
A