physiology of hearing ppt

81
PHYSIOLOGY OF HEARING BY: Dr.Humra shamim

Upload: humra-shamim

Post on 11-Apr-2017

42 views

Category:

Health & Medicine


4 download

TRANSCRIPT

Page 1: Physiology of hearing ppt

PHYSIOLOGY OF HEARING

BY: Dr.Humra shamim

Page 2: Physiology of hearing ppt

IS HEARING IMPORTANT? Communication: hearing is essential to

language Localisation: determination of location

of unseen sound sources

Page 3: Physiology of hearing ppt

WHAT IS REQUIRED FOR NORMAL HEARING?

Adequate stimulus (sound) Conduction of stimulus to sensory

organ of hearing Sensory transduction of stimulus at

organ of hearing Neural transmission of the signal Central auditory processing of the

signal at brain

Page 4: Physiology of hearing ppt

SOUND Sound is a form of energy that propagates in the form

of waves The speed of sound depends on the medium through

which the wave passes. Speed of sound in air is 343m/s in water is 1482m/sec The sound frequencies audible to humans range from

about 20 to 20,000 cycles per second (cps, Hz). sound intensity is expressed by taking the logarithmic

ratio of two sound intensities (the numerator being the sound intensity of interest, and the denominator being a reference sound intensity) and multiplying by 10.

dB = 10 log10 J/Jr, where J is the intensity of the sound of interest, and Jr is the intensity of reference

Page 5: Physiology of hearing ppt

TECHNICAL JARGON:

•Strength of the sound•Loudness denotes the appreciation of sound intensity•Expressed in decibel (dB)

Amplitude/loudness

•Number of cycles per second•Pitch /Tone denotes the appreciation of frequency•Expressed in Hertz(Hz)

Frequency/pitch /tone

•Resistance offered by a medium to sound wavesImpedance

Page 6: Physiology of hearing ppt

INTENSITY Intensity is defined as the power transmitted

by sound wave a unit area. Intensity is dependent on pressure and

velocity average taken over whole cycle Intensity =peak pressure x peak velocity/2 Displacement produced by sound waves vary

with frequency if the intensity is constant Low frequency vibrations produce greater

displacements

Page 7: Physiology of hearing ppt

Simple harmonic motion. Simple harmonic motion is a periodic motion that undulates around a null point with equalamplitudes. The amplitude is the maximum amount of displacement from the null point in one direction. The frequency of a simple harmonic motion is the number of cycles per second, and is measured in Hertz (Hz). The period of a cycle is the inverse of its frequency (1/f), and represents the duration of a single cycle

Page 8: Physiology of hearing ppt

HUMAN AUDITORY FIELD

The human ear is sensitive to sound over wide range of amplitudes:0.0002—200 dyne/cm2

It can detect the difference between two sounds occuring 10micro seconds apart in time.

Page 9: Physiology of hearing ppt

EAR ACTS AS A TRANSDUCER

SOUNDENERGY

MECHANICAL ENERGY

ELECTRICAL ENERGY

Page 10: Physiology of hearing ppt

NATURAL RESONANT FREQUENCYEXTERNAL AUDITORY CANAL--------------- 3000Hz

TYMPANIC MEMBRANE----------------------- 800-1600Hz

MIDDLE EAR---------------------------------------- 800Hz

OSSICULAR CHAIN------------------------------ 500-2000Hz

Page 11: Physiology of hearing ppt

FUNCTIONS OF EXTERNAL EAR:

Sound collection

Increasing pressure on tympanic

membrane in a frequency sensitive

way

Sound localisation

Page 12: Physiology of hearing ppt

EXTERNAL EAR Act as a resonator It increases the

pressure at the ear drum in a frequency sensitive way

Helps in localisation of direction of sound

Page 13: Physiology of hearing ppt

SOUND COLLECTION Pinna- concha system catches sound over large area

and concentrate it to smaller area of ext. auditory meatus.

This increases the total energy available to the tympanic membrane

Page 14: Physiology of hearing ppt

FEATURES OF EXTERNAL CANAL Open on one end only The impedance of ear drum is about 3-

4times more than air 30% of incident energy gets reflected

from external canal Efficient in conducting sound in frequency

range of 3-5kHz Cuts off unwanted frequency helping in

better speech discrimination

Page 15: Physiology of hearing ppt

PRESSURE INCREASE BY EAC If a tube which is closed at one end and open at

other is placed in a sound field then pressure is low at open end and high at closed end.

This phenomenon is seen in EAC at 3kHz frequency , and at concha at 5kHz

The two main resonance are complementary , and increases sound pressure in range of 2-7kHz.

Page 16: Physiology of hearing ppt

SOUND LOCALISATION: Because of its shape, the pinna shield the

sound from rear end,change timbre,and helps to localize sound from in front or back

Cues for sound localization from right/left Sound wave reaches the ear closer to

sound source before it arise in farthest ear Sound is less intense as it reaches the

farthest ear because head act as barrier Auditory cortex integrates these cues to

determine location

Page 17: Physiology of hearing ppt

TOTAL GAIN The total effect of reflection of sound from

head,pinna and external canal resonances is to add 15-20dB to sound pressure, over frequency range of 2-7kHz.

Page 18: Physiology of hearing ppt

FUNCTIONS OF MIDDLE EAR: Couples sound energy to the cochlea Impedance matching Attenuation reflex Physically protects the cochlea Phase differential effect :Couples sound

preferentially to only one window ,thus producing a differential pressure between the windows required for the movement of cochlear fluid

Page 19: Physiology of hearing ppt

IMPEDANCE TRANSFORMER Impedance is defined as the resistance

offered by a medium for transmission of sound

middle ear acts as impedance transformer

Cochlear fluids have an impedance equall that of sea water (1.5X10 N.sec/m3)

Page 20: Physiology of hearing ppt

IMPEDANCE TRANSFORMER Impedance is defined as the resistance offered by a

medium for transmission of sound Middle ear ossicles are suspended by ligaments Axis of rotation of ossicles and axis of suspension by

ligaments virtually coincides with their centre of inertia At low frequencies the ligaments play an important role

in maintaining ossicular positions(elastic effect) Middle ear converts the low pressure high displcement

vibrations of ear drum into high pressure low displacement vibrations this is suitable to drive cochlear fluids

Page 21: Physiology of hearing ppt

IMPEDANCE MISMATCH

IF THERE WAS NO MIDDLE EAR SYSTEM ,99% OF SOUND WAVES WOULD HAVE REFLECTED BACK FROM OVAL WINDOW

MIDDLE EAR BY ITS IMPEDENCE MATCHING PROPERTY ALLOWS 60% OF SOUND ENERGY TO DISSIPATE IN INNER EAR

Page 22: Physiology of hearing ppt

IMPEDANCE EFFICIENCY Only 60%of sound energy from TM gets

transmitted &absorbed in the cochlea Without the middle ear only 1%of

sound energy will be absorbed by the cochlea

Page 23: Physiology of hearing ppt

LOW FREQUENCY SOUND DAMPENERS

Middle ear efficiency is the best at 1kHz There is transmission loss of low

frequency sounds due to elastic stiffness of middle ear ligaments(annular ligament is the most important)

Air inside middle ear cavity also dampens low frequency sound transmission

Grommet insertion improves transmission of low frequency sounds

Page 24: Physiology of hearing ppt

“IMPEDANCE MATCHING” BY THE MIDDLE EAR SYSTEM

The shape of tympanic membrane

The lever action of middle ear ossicles

Area of tympanic membrane relative to oval window

Page 25: Physiology of hearing ppt

A) AREA OF THE TYMPANIC MEMBRANE RELATIVE TO OVAL WINDOW

Total effective area of tympanic membrane 69mm2

Area of stapes footplate is 3.2mm2

Effective areal ratio is 14:1 Thus by focusing sound

pressure from large area of tympanic membrane to small area of oval window the effectiveness of energy transfer between air to fluid of cochlea is increased

Page 26: Physiology of hearing ppt

B) LEVER ACTION OF EAR OSSICLESHandle of malleus is

1.3 times longer than long process of incus

Overall this produces a lever action that converts low pressure with a long lever action at malleus handle to high pressure with a short lever action at tip of long process of incus

Page 27: Physiology of hearing ppt

C) SHAPE OF THE TYMPANIC MEMBRANE TM buckles as it

moves to and fro This reduces

malleolar movement

TM thus acts as a mechanical lever

This causes high pressure low displacement system

Page 28: Physiology of hearing ppt

HYDRAULIC ACTION OF TYMPANIC MEMBRANE

The most important factor in the middle ear's impedance matching capability comes from the “area ratio” between the tympanic membrane and the stapes footplate

Total area of tympanic membrane 90mm2 Functional area of tympanic membrane is two third

(69mm2).Area of stapes footplate is 3.4mm2.So , Effective areal ratio is 14:1 Thus by focusing sound pressure from large area of

tympanic membrane to small area of oval window the effectiveness of energy transfer between air to fluid of cochlea is increased

Page 29: Physiology of hearing ppt

ACTION OF TYMPANIC MEMBRANE Eustachian tube equilibriates the

air pressure in middle ear with that of atmospheric pressure,thus permitting tympanic membrane to stay in its most neutral position.

A buckling motion of tympanic membrane result in an increased force and decreased velocity to produce a fourfold increase in effectiveness of energy transfer

Page 30: Physiology of hearing ppt

Total transformer ratio=14x1.3=18.2:1

The combined effects of the area ratio and the lever ratio give the middle ear output a 28-dB gain theoretically. In reality, the middle ear sound pressure gain is only about 20 dB; this is mostly due to the fact that the tympanic membrane does not move as a rigid diaphragm

Page 31: Physiology of hearing ppt

PHASE DIFFERENTIAL EFFECT Sound waves striking the tympanic membrane

do not reach the oval and round window simultaneously.

There is preferential pathway to oval window due to ossicular chain.

This acoustic separation of windows is achieved by intact tympanic membrane and a cushion of air around round window

This contributes 4dB when tympanic membrane is intact

Page 32: Physiology of hearing ppt

ROLE OF MIDDLE EAR MUSCLES: TENSOR TYMPANI MUSCLE

ATTACHES TO THE HANDLE OF MALLEUS.IT PULLS THE DRUM MEDIALLY.

STAPEDIUS MUSCLE ATTACHES TO THE POSTERIOR ASPECT OF STAPES

CONTRACTION OR THESE MUSCLE INCREASES THE STIFFNESS OF OSSICULAR CHAIN THUS BLUNTING LOW FREQUENCIES

DECREASES A PERSON’S SENSITIVITY TO THEIR OWN SPEECH

Page 33: Physiology of hearing ppt

PROTECTIVE FUNCTIONS OF MIDDLE EAR MUSCLES

Stapedius contraction can reduce transmission by upto 30dB for frequencies less than 1-2 kHz. for higher frequencies this is limited to 10dB.

Only the stapedius muscle contracts in response to loud noise in humans

The whole stapedial reflex arc has 3-4 synapses

Stapedial reflex latency is 6-7ms

Page 34: Physiology of hearing ppt

ATTENATION REFLEX When loud sounds are transmitted through the

ossicular system and from there into the central nervous system, a reflex occurs after a latent period of only 40 to 80 ms to cause contraction of the stapedius muscle and the tensor tympani muscle

The tensor tympani muscle pulls the handle of the malleus inward while the stapedius muscle pulls the stapes outward. These two forces oppose each other and thereby cause the entire ossicular system to develop increased rigidity, thus greatly reducing the ossicular conduction of low frequency sound

Page 35: Physiology of hearing ppt

DAMAGED MIDDLE EAR SCENARIOS Damaged middle ear can cause loss of

transformer mechanism Differntial pressure levels between the two

windows could not be maintained Scala vestibuli is more yielding than scala tympani

.differential movements of fluid is still possible . Small compliance of annular ligament in

comparison to much larger compiant round window could again cause differential pressure

Page 36: Physiology of hearing ppt

BONE CONDUCTION Normal route for hearing some

component of one’s own voice Useful in cases of severe conductive

losses Can be used as a diagnostic tool

Page 37: Physiology of hearing ppt

BONE CONDUCTION INNER EAR FACTORS: Intrinsic detection of distortional vibrations of

cochlear bone Differential distortion of bony structures of

cochlea(s.vestibuli is larger than s.tympani )could cause movement of cochlear fluid

Direct vibration of osseous spiral lamina Direct transmission of vibrations from the skull

via CSF to the cochlear fluids Leaving one window open improved sound

conduction

Page 38: Physiology of hearing ppt

BONE CONDUCTION MIDDLE EAR FACTORS

Vibration of the skull faithfully transmitted to the ossicles of middle ear cavity

Inertia of middle ear ossicles doesn’t coincide with their point of attachment

Middle ear acts as a band pass filter with peak transmission around 1kHz

This accounts for carharts notch though at a slightly higher frequency

Page 39: Physiology of hearing ppt

BONE CONDUCTION EXTERNAL EAR FACTORS:

Bone vibrations are conducted through the external canal and the air within it

Vibrations can escape externally if the canal is open

Occlusion of external ear increases bone conduct ion

External radiation of sound is best for low frequencies, hence change with occlusion Is greatest for these frequencies.

Page 40: Physiology of hearing ppt

INNER EAR PHYSIOLOGY The two important functions of the inner ear are

HEARING and BALANCE.

The portion of the inner ear that deals with hearing is the cochlea, and that deals with balance is collectively known as the vestibular organs (semicircular canals, utricle, and saccule).

COCHLEA acts as a TRANSDUCER that translates sound energy into a form suitable for stimulating the dendrites of auditory nerve.

Page 41: Physiology of hearing ppt

STRUCTURE OF COCHLEA:

The cochlea is a fluid-filled space with three compartments: scala tympani, scala media, and scala vestibuliThe scala tympani and the scala media are separated by the basilar membrane, and the scala media and the scala vestibuli are separated by Reissner's membrane.The scala media contains the organ of Corti which contains inner and outer hair cells

Page 42: Physiology of hearing ppt

The inner hair cells are flask-shaped cells,3000 approx in number and arranged in a single row

the outer hair cells are cylindrical-shaped,12000 approx in number arranged in 3-4 rows

The hair cells derive their names from having hairlike projections on their apical surface. These hair like projections are stereocilia, which play an important role in the signal transduction properties of the hair cells

Page 43: Physiology of hearing ppt

ENDOLYMPH Formed by stria vascularis Endolymphatic sac maintains

homeostsis of endolymph It has a high sodium and low potssium

content Endolymph has positive potential

gradient +50-120mv(endocochlear potential)

Na k ATPase is responsible for this gradient.

Page 44: Physiology of hearing ppt

PERILYMPH: Site of production is controversial ?CSF Occupies perilymphatic space. continuous

between vestibular &cochlear divisions Ionic concentration resembles extracellular

fluid Perilymph from s.vestibuli originates from

plasma ,while perilymph from s.tympani originates from plasma and CSF

Electric potential of s.tymapani is 7mv and s. vestibuli is +5mv

Page 45: Physiology of hearing ppt

BASILIAR MEMBRANE Separates s.media from s .tympani Length’s of basilar membrane increases

progressively from oval window to the apex (0.04mm near oval window and 0.5mm at helicotrema )12 fold increase

Diameters of basilar fibres decrease from oval window to helicotrema

The stiff short fibres near the oval window vibrate best at very high frequency,while long limber fibres near the tip of cochlea vibrate best at a low frequency.

Page 46: Physiology of hearing ppt

Schematic cross-sectional view of the human cochlea. The scala media (cochlear duct) is filled with endolymph, and the scala vestibuli and tympani are filled with perilymph. The endolymph of the scala media bathes the organ of Corti, located between the basilar and tectorial membranes and containing the inner and outer hair cells. Hair cells contain stereocilia along the apical surface and are connected by tip links. In response to mechanical vibration of the basilar membrane, deflection of stereocilia, displacement of tip links, and opening of gated potassium channels. Epithelial supporting cells (connexin channels, red) allow for the flow of potassium ions

Page 47: Physiology of hearing ppt

The scala vestibuli and the scala tympani are filled with perilymph, which has a low potassium concentration.

The scala media is filled with endolymph, which has a high potassium concentration.

The unique electrolyte composition of the scala media sets up a large electrochemical gradient, called the endocochlear potential, which is about +80 mV relative to perilymph. The maintenance of such a large electrochemical gradient is performed by the stria vascularis

Page 48: Physiology of hearing ppt

ENDOCOCHLEAR POTENTIAL

The importance of is that the tops of hair cells project through the reticular lamina and are bathed by the endolymh of the scala media ,whereas perilymph bathes the lower bodies of the hair cells. further more the hair cells have a negative intracellular potential of -70mv wrt the perilymphbut -150mv wrt endolymph at their upper surfaces where the hair cells project through the reticular lamina and into the endolymph

Page 49: Physiology of hearing ppt

COCHLEAR MECHANICS: Mechanical travelling wave

in the cochlea is the basis of frequency selectivity

The travelling wave reaches a peak and dies away rapidly

As the wave moves up the cochlea towards its peak ,it reaches a region in which the membrane is mechanically active. In this region the membrane stars putting energy into the wave .the amplitude raises rapidly only to fall rapidly.

Page 50: Physiology of hearing ppt

TRAVELLING WAVE THEORY The movements of the

footplate of the stapes set up a series of traveling waves in the perilymph of the scala vestibuli

High-pitched sounds generate waves that reach maximum height near the base of the cochlea; low-pitched sounds generate waves that peak near the apex

The basilar membrane is not under tension, and it also is readily depressed into the scala tympani by the peaks of waves in the scala vestibuli

Page 51: Physiology of hearing ppt

Schematic showing sound propagation in the cochlea. As sound energy travels through the external and middle ears, it causes the stapes footplate to vibrate. The vibration of the stapes footplate results in a compressional wave on the inner ear fluid. Because the pressure in the scala vestibuli is higher than the pressure in the scala tympani, this sets up a pressure gradient that causes the cochlear partition to vibrate as a traveling wave. Because the basilar membrane varies in its stiffness and mass along its length, it is able to act as a series of filters, responding to specific sound frequencies at specific locations

Page 52: Physiology of hearing ppt

HAIR CELLS: The hairs ends of the OUTER HAIR

CELLS are fixed tightly in a rigid structure composed of a flat plate, called the reticular lamina, supported by triangular rods of Corti,which are attached tightly to the basilar fibers.

The hairs of the INNER HAIR CELLS are not attached to the tectorial membrane, but they are apparently bent by fluid moving between the tectorial membrane and the underlying hair cells.

Page 53: Physiology of hearing ppt

INNER HAIR CELLS Makes large no. of synaptic contact with afferent

fibres of auditory neve 95% of afferent auditory nerves make contact with

inner hair cells Detects basilar membrane movement Tips of inner hair cells are not embedded in the

tectorial membrane as outer hair cells They fit loosely into a groove called “henson’s groove” They are driven by viscous drag of endolymph inner hair cells respond to the velocity rather than

displacement of basilar membrane

Page 54: Physiology of hearing ppt

OUTER HAIR CELLS Very few outer hair cells synapse with

auditory nerves Inside of outer hair cells have -70 mV They serve to amplify basilar membrane

vibration They increase the sensitivity and

selectivity of cochlea Cochlear microphonics are derived from

these cells

Page 55: Physiology of hearing ppt

RESTING POTENTIAL OF HAIR CELLS Each hair cell has an intracellular potential of (-

70mV) with respect to perilymph. At upper end of hair cell the potential difference

between intracellular fluid and endolymph is (-150mV)

This high potential difference makes the cell very sensitive. Tip links

The tops of the shorter stereocilia are attached by thin filaments to the back sides of their adjacent longer stereocilia

Page 56: Physiology of hearing ppt

The basilar fibers, the rods of Corti, and the reticular lamina move as a rigid unit

Upward movement of the basilar fiber rocks the reticular lamina upward and inward toward the modiolus.Then, when the basilar membrane moves downward, the reticular lamina rocks downward and outward.

The inward and outward motion causes the hairs on the hair cells to shear back and forth against the tectorial membrane.Thus, the hair cells are excited whenever the basilar membrane vibrates

Page 57: Physiology of hearing ppt

Schematic showing the role of tip links in hair cell signal transduction

As the stereocilia is deflected toward the direction of the tallest row, it causes the tip links to stretch. The stretch of the tip links causes the opening of stretch-sensitive cationic channels located on the stereocilia

The opening of these stretch-sensitive cationic channels on the stereocilia causes a large influx of cationic current, which leads to hair cell depolarization.

As the stereocilia is deflected away from the tallest row, it causes a relaxation of the tip links, which decreases the probability of ion channel opening. This leads to hyperpolarization of the hair cell

Page 58: Physiology of hearing ppt

DEPOLARIZATION/ACTIVATION When the cilia are bent

in the direction of the longer ones, the tips of the smaller stereocilia are tugged outward.This causes a mechanical transduction that opens 200 to 300 cation-conducting channels, allowing rapid movement of potassium ions from the surrounding scala media fluid into the stereocilia, which causes depolarization of the hair cell membrane

Page 59: Physiology of hearing ppt

The influx of potassium inside the cell causes activation of calcium channels

This calcium drags the neurotransmitter filled vesicle to fuse with cell membrane at base of cell.

Neurotransmitter (glutamate)releases and excites the dendrites of afferent nerve fibres.

Page 60: Physiology of hearing ppt

CENTRAL AUDITORY PATHWAY

Inputs from auditory nerve drive multiple cell types in different subdivisions of the cochlear nucleus, with each cell type projecting centrally to different targets in the superior olivary complex, lateral lemniscus nuclei, and inferior colliculus

Cochlear nucleus is the critical first relay station for all ascending auditory information originating in the ear, and is located in the pontomedullary junction its major subdivisions: the dorsal cochlear nucleus, the anterior ventral cochlear nucleus, and the posterior ventral cochlear nucleus

Cochlear nuclei

Superior olivary

complex

Nucleus of

lateral lemnisc

us

Inferior colliculu

s

Medial geniculte body

Auditory cortex

Page 61: Physiology of hearing ppt

nerve fibers from the spiral ganglion of Corti enter the dorsal and ventral cochlear nuclei

second-order neurons pass mainly to the opposite side of the brain stem to terminate in the superior olivary nucleusthe superior olivary

nucleus,the auditory pathway passes upward through the lateral lemniscus.

Page 62: Physiology of hearing ppt

Some of the fibres terminate in the nucleus of lateral lemniscus ,but many bypass this nucleus and travel on to the inferior colliculus,where all or almost all the auditory fibres synapse

From there the pathway passes to the medial geniculate nucleus,where all the fibres do synapse

Finally the pathway proceeds by way of the auditory radiations to auditory cortex.

Page 63: Physiology of hearing ppt

The lateral lemniscus is formed by the three fiber tracts from the cochlear nucleus

The inferior colliculus located in the midbrain just caudal to the superior colliculus.

receives projections directly from the cochlear nucleus and information about interaural time and amplitude differences from the medial superior olive and lateral superior olive

processes the information it receives and sends fibers to the medial geniculate body of the thalamus.

.

Functional magnetic resonance imaging showing the ascending pathways of auditory processing from the auditory brainstem to the auditory cortex

Page 64: Physiology of hearing ppt

THE MEDIAL GENICULATE

BODY

is the thalamic auditory relay center that receives auditory information from the inferior colliculus.

It has three divisions: ventral, dorsal, and medial.

Plays an important role in sound localization and processing of complex vocal communications, such as human speech

AUDITORY CORTEX The main auditory portion of the

cerebral cortex resides in the temporal lobe, close to the sylvian fissure

The primary auditory cortex is located on the superior surface of the temporal lobe (Heschl's gyrus). This is also known as area A1, and corresponds to Brodmann's area 41.

Page 65: Physiology of hearing ppt

The auditory association cortex is also known as area A2, and corresponds to Brodmann's areas 22 and 42.

The primary auditory cortex is directly excited by projections from medial geniculate body,whereas the auditory associaton area are excited by impulses from primary auditory cortex as well as some projections thalamic association areas adjacent to MGB

the primary auditory cortex is tonotopically tuned, with high frequencies being represented more medially, and low frequencies being represented more laterally

FUNCTIONS integrating and processing complex auditory

signals, including language comprehension the auditory association cortex plays an

important role in speech perception auditory association cortex is located lateral

to the primary auditory cortex, and it is part of a language reception area known as Wernicke's area

Page 66: Physiology of hearing ppt

FUNCTIONS OF AUDITORY CORTEX Perception of sound

Judging the intensity of the sound

Analysis of different properties of sound

Page 67: Physiology of hearing ppt

PECULARITIES OF AUDITORY PATHWAY

First ,signals from both ears are transmitted through the pathways of both sides of the brain ,with a preponderance of transmission in the contralateral pathway

Second ,many collateral fibres from the auditory tracts pass directly into the reticular activating system of the brain stem

Third ,a high degree of spatial orientation is maintained in the fibre tracts from the cochlea all the way to the cortex

Page 68: Physiology of hearing ppt

DETERMINATION OF LOUDNESSDetermined by the auditory system in at least three

ways. First, as the sound becomes louder, the amplitude of

vibration of the basilar membrane and hair cells also increases, so that the hair cells excite the nerve endings at more rapid rate

Second, as the amplitude of vibration increases, it causes more and more of the hair cells on the fringes of the resonating portion of the basilar membrane to become stimulated, thus causing spatial summation of impulses.

Third, the outer hair cells do not become stimulated significantly until vibration of the basilar membrane reaches high intensity, and stimulation of these cells presumably apprises the nervous system that the sound is loud.

Page 69: Physiology of hearing ppt

DETERMINATION OF SOUND FREQUENCY—THE “PLACE” PRINCIPLE There is spatial organization of the nerve fibers in the cochlear

pathway, all the way from the cochlea to the cerebral cortex Specific brain neurons are activated by specific sound

frequencies The major method used by the nervous system to detect

different sound frequencies is to determine the positions along the basilar membrane that are most stimulated. This is called the place principle

Page 70: Physiology of hearing ppt

AUDITORY NERVE FIBRES: Inner hair cells excite auditory nerves Sound stimulus, transmittor release

and action potential generation occur in synchrony (phase locking)

Commonly seen at low frequencies

Page 71: Physiology of hearing ppt

FREQUENCY CODING AT AUDITORY NERVE Phase locking Temporal properties (timing of action

potential) Frequency selectivity(place coding)

Page 72: Physiology of hearing ppt

THEORIES OF HEARING Place theory of Helmholtz Temporal theory of Rutherford Volley theory of Wever Place theory of Lawrence Travelling wave theory of Bekesy

Page 73: Physiology of hearing ppt

PLACE THEORY Acc to helmholtz basilar memebrane

has different segments that respond to different frequencies

Sharply tuned resonators dampen slowly this could cause after ringing cessation of stimuli

This theory fails to explain why a stream of clicks of frequencies ranging from 1220,1300 and 1400 Hz is heard as 1000 Hz

Page 74: Physiology of hearing ppt

TELEPHONIC THEORY Rutherford proposed that entire cochlea responds

as a whole to all freqquencies instead of being activated on a plate by place basis.

Here the sound of all frequencies are transmitted as in a telephone cable and frequency analysis is done at a higher level(brain)

Damage to certain portion of cochla can cause preferential loss of hearing certain frequencies i.e. like damage to the basal turn of cochlea causing inability to hear high frequency sounds

This cannot be explained by telephonic theory.

Page 75: Physiology of hearing ppt

VOLLEY THEORY Proposed by Wever Several neurons acting as a group can

fire in response to high frequency sound even though none of them could do it individually

Page 76: Physiology of hearing ppt

PLACE VOLLEY THEORY Proposed by lawrence Combines both volley and place theory This theory thus attemps to explain

sound transmission and perception

Page 77: Physiology of hearing ppt

TRAVELLING WAVE THEORY Proposed by bekesy This theory proposes frequency coding

to take place at the level of cochlea. High frequencies are represented

towards the base while lower frequencies are closes to apex

Page 78: Physiology of hearing ppt

TUNING BY OUTER HAIR CELLS Tuning of sound in basilar membrane requires local

addition of mechanical energy

There are efferent fibres from crossed olivocochlear bundle supplying the outer cells

The inputs from these bundle causes contraction of outer cells located close to maximum of travelling wave give rise to extra distortion of basilar membrane

This provides an extra gain of 40-50dB to the system

Page 79: Physiology of hearing ppt

CENTRIFUGAL INNERVATION OF COCHLEA Cochlea recieves centrifugal or efferent

nerve supply,i.e. olivococchlear bundle It reduces the magnitude of travelling

wave ,and possibly protects the ear against moderate level of noise damage

Reduces the masking effect of background noise in complex tasks

Page 80: Physiology of hearing ppt

COCHLEAR ECHOES/OTOACOUSTIC EMISSIONS

Energy produced by outer hair cell motility serves as an amplifier within the cochlea, contributing to better hearing

OAEs are produced by the energy from outer hair cell motility that makes its way outward from the cochlea through the middle ear, vibrating the tympanic membrane, and propagating into the external ear canal

Page 81: Physiology of hearing ppt

THANK YOU