Physics of Hearing The Lecture 2023
Physics of Hearing The Lecture 2023
Physics of Hearing The Lecture 2023
Ossicles and middle ear: There are three ossicles in the middle ear the malleus, incus and stapes. The malleus has head,
neck, handle (manubrium), a lateral and an anterior process. The incus has a body and a short process, and a long process
which hangs vertically and attaches to the head of stapes. The stapes has a head, neck, anterior and posterior crura,and a
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footplate. The footplate is held in the oval window by annular ligament. The ossicles conduct sound energy from the
tympanic membrane to the oval window and then to the inner ear fluid.
The physiology of the auditory system is complex, and our understanding of how the system functions is not yet complete.
Complete understanding of the auditory system also requires knowledge of the nature of sound and the function of the
structures.
Acoustics
Acoustics is the science that is concerned with the production, control, transmission, reception, and effects of sound.
Sound is energy: mechanical radiant energy that is transmitted through pressure waves in a material medium (e.g., air,
water, metal). In the case of hearing, sound is the sensation perceived by the ear.
This sound energy is captured by the outer ear, transformed by the middle ear, and transduced by the inner ear. Sound is
described in terms of its basic physical attributes: frequency, intensity, and time/phase of the vibration. These physical
attributes also have psychological correlates, which are pitch, loudness, and quality, respectively.
Frequency
A single-frequency sound, or pure tone, is the standard used in the assessment of auditory sensitivity (threshold).
Frequency is a physical attribute of a sound and is defined as the number of cycles per unit of time. Although measured
in cycles per second, frequency is reported in hertz (Hz) (Fig 3). Video1
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Period refers to the amount of time it takes for one cycle to occur; therefore, period is the reciprocal of frequency (period
=1/frequency). This 1,000-Hz tone would have a period of 1/1,000 seconds. Wavelength (λ) is the distance sound travels
in one period and is reported in centimeters, feet, or miles, depending on how the velocity is recorded (Fig 4). Video2
Fig.3 Graphs of two sine waves of different frequencies plotted over time. The top graph is a low frequency (1,000 Hz)
and the bottom is a higher frequency (4,000 Hz) as denoted by the number of cycles in the same time window.
Fig 4 Wavelength
The number of times an object vibrates determines its frequency, but how far the object moves determines its intensity.
Intensity or amplitude then becomes another physical attribute of sound. Intensity relates to the strength of a sound as
shown in Fig. 5; the distance a mass moves from the point of rest is the amplitude of the sound. Intensity is usually
measured in decibels (dB).
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Fig. 5 Graphs of two sine waves of the same frequency (1,000 Hz) but different intensities plotted over time. The tones
have the same cycles per second but differ in the amplitude of the waves.
Phase
The phase of a sound refers to the relative timing of sound waves. It is simplest to refer to the starting phase of the signal.
Therefore, at time zero the point of the sine wave where the signal begins will be the starting phase.
Resonance refers to the phenomenon whereby one body can be set into motion by the vibration of another body. If a
given area has a “resonant frequency,” then that frequency is amplified when it is presented in that area. In other words,
there is an increase in the intensity of that signal because the surface of the area with the resonant frequency vibrates at the
particular frequency that has been presented and therefore increases its intensity. Video 3
Physiology of Hearing
The natural or usual manner by which humans detect sound is via an airborne or acoustic signal. Once the sound is
generated, it travels through the air in a disturbance called a sound wave. The flange and concha of the pinna collect,
amplify, and direct the sound wave to the tympanic membrane by the external auditory meatus.
At the tympanic membrane, several transformations of the signal occur: (1) the acoustic signal becomes mechanoacoustic;
(2) it is passed along to the ossicular chain.
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Transformation and the Middle Ear Mechanism
The overall middle ear transformer ratio is the product of 1.3 × 17, or a transformer ratio of 22:1 due to the combined area
effect of the drum and lever ratio of the ossicles. This equates to approximately 27 dBof gain and when combined with the
action of the external ear will compensate for the loss of energy due to the impedance mismatch.
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Fig 6 Transformation and the Middle Ear Mechanism
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ASSESSMENT OF HEARING
Figure 7 Two-room audiometry setup. Audiometrician watches responses of the patient sitting across a glass partition.
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Clinical applications
Hearing loss can be of three types:
1. Conductive hearing loss. It is caused by any disease process interfering with the conduction of sound from the external
ear to the stapediovestibular joint. Thus the cause may lie in the external ear (obstructions), tympanic membrane
(perforation), middle ear (fluid), ossicles (fixation or disruption) or the eustachian tube (obstruction).
2. Sensorineural (SN) hearing loss. It results from lesions of the cochlea (sensory type) or VIIIth nerve and its central
connections (neural type). The term retrocochlear is used when hearing loss is due to lesions of VIIIth nerve, and central
deafness, when it is due to lesions of central auditory connections.
3. Mixed hearing loss. In this type, elements of both conductive and sensorineural deafness are present in the same ear.
There is air-bone gap indicating conductive element, and impairment of bone conduction indicating sensorineural loss.
Mixed hearing loss is seen in some cases of otosclerosis and chronic suppurative otitis media.
Objective test to assess the middle ear mechanism (Impedance and admittance)
Tympanometry. It is based on a simple principle, i.e. when a sound strikes tympanic membrane, some of the sound
energy is absorbed while the rest is reflected. A stiffer tympanic membrane would reflect more of sound energy than a
compliant one. By changing the pressures in a sealed external auditory canal and then measuring the reflected sound
energy, it is possible to find the compliance or stiffness of the tympano-ossicular system and thus find the healthy or
diseased status of the middle ear.
Essentially, the equipment consists of a probe which snugly fits into the external auditory canal and has three channels:
(i) to deliver a tone of 220 Hz, (ii) to pick up the reflected sound through a microphone and (iii) to bring about changes in
air pressure in the ear canal from positive to normal and then negative (Figure 9). By charting the compliance of tympano-
ossicular system against various pressure changes, different types of graphs called tympanograms are obtained which are
diagnostic of certain middle ear pathologies.
Figure 9 Principle of impedance audiometry. (A) Oscillator to produce a tone of 220 Hz. (B) Air pump to increase or
decrease air pressure in the air canal. (C) Microphone to pick up and measure sound level reflected from the tympanic
membrane.
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Figure 10 Types of tympanograms.
A—Normal.
As—Reduced compliance at ambient pressure (otosclerosis). ‘s’ stands for shallow tympanogram but remember for
stiffness.
Ad—Increased compliance at ambient pressure (ossicular discontinuity). ‘d’ stands for deep tympanogram. Remember
disruption of ossicular chain.
B—Flat or dome-shaped (fluid in middle ear).
C—Maximum compliance at pressures more than −200 mm H2O
(negative pressure in middle ear), e.g. eustachian tube obstruction or early stage of otitis media with effusion.