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Physiology of Hearing & Equilibrium Dr. Vishal Sharma

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Page 1: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Physiology of Hearing &

EquilibriumDr. Vishal Sharma

Page 2: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Parts of hearing apparatus

Conductive apparatus: external & middle ear

Conducts mechanical sound impulse to inner ear

Perceptive apparatus: cochlea

Converts mechanical sound impulse into electrical

impulse & transmits to higher centers

Page 3: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Role of external ear

• Collection of sound waves by pinna &

conduction to tympanic membrane

• Increases sound intensity by 15-20 dB

• Cupping of hand behind pinna also increases

sound intensity by 15 dB especially at 1.5 kHz.

Page 4: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 5: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Role of middle ear in hearing

• Impedance matching mechanism (step – up

transformer or amplifier function)

• Preferential sound pressure application to oval

window (phase difference by ossicular coupling)

• Equalization of pressure on either sides of

tympanic membrane (via Eustachian tube)

Page 6: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Impedance matching mechanism

• When sound travels from air in middle ear to fluid in

inner ear, its amplitude is ed by fluid impedance.

• Only 0.1 % sound energy goes inside inner ear.

• Middle ear amplifies sound intensity to compensate

for this loss. Converts sound of low pressure, high

amplitude to high pressure, low amplitude vibration

suitable for driving cochlear fluids.

Page 7: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Hermann von Helmholtz

Described impedance matching in 1868

Page 8: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

T.M. Catenary lever (curved membrane effect):

Sound waves focused on malleus. Magnifies 2 times

Ossicular Lever ratio:

Length of handle of malleus > long process of incus.

Magnifies 1.3 times

Surface area ratio (Hydraulic lever):

T.M. = 55 mm2 ; Stapes foot plate = 3.2 mm2

Magnifies 17 times

Total Mechanical advantage: 2 X 17 X 1.3 = 45

times = 30 – 35 dB

Page 9: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 10: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 11: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 12: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

• Property to allow certain sound frequencies to pass more readily to inner ear.

• External auditory canal = 2500 – 3000 Hz

• Tympanic membrane = 800 - 1600 Hz

• Ossicular chain = 500 – 2000 Hz

• Range = 500 – 3000 Hz (speech frequency)

Natural Resonance

Page 13: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 14: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Preferential sound pressure application (phase difference)

• Sound pressure preferentially applied to oval

window by ossicular coupling while round

window is protected by tympanic membrane

• Sound pressure travels to scala vestibuli

helicotrema scala tympani round window

membrane yields scala media moves up &

down movement of hair cells in scala media

Page 15: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Preferential sound pressure application (phase difference)

• Yielding of round window membrane (push-pull

effect) is necessary as inner ear fluids are

incompressible

• Large tympanic membrane perforation loss of

this function (push-push effect) no movement

of inner ear fluids

Page 16: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 17: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Ossicular break + intact T.M. = 55-60 dB loss

Ossicular break + T.M. perforated = 45-50 dB loss

Page 18: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 19: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 20: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

– Movement of basilar membrane

– Shear force between tectorial membrane & hair cells

– Cochlear microphonics

– Nerve impulses

Transduction of mechanical energy to electrical impulses

Page 21: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 22: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 23: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Cochlear hair cells

Page 24: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 25: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
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Page 28: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Transducer Mechanism

Page 29: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 30: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Auditory pathway• Eighth (Auditory) nerve

• Cochlear nucleus

• Olivary nucleus (superior)

• Lateral lemniscus

• Inferior colliculus

• Medial geniculate body

• Auditory cortex

Page 31: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 32: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
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Page 34: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 35: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 36: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 37: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 38: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Theories of hearingPlace / Resonance Theory (Helmholtz, 1857)

Perception of pitch depends on selective

vibration of specific place on basilar membrane.

Telephone Theory (Rutherford, 1886)

Entire basilar membrane vibrates. Pitch related

to rate of firing of individual auditory nerve

fibers.

Page 39: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Theories of hearingVolley Theory (Wever, 1949)

> 5 KHz: Place theory; <400 Hz: Telephone theory

400 – 5000 Hz: Volley theory

Groups of fibres fire asynchronously (volley

mechanism). Required frequency signal is

presented to C.N.S. by sequential firing in groups

of 2 - 5 fibers as each fiber has limitation of 1 Khz.

Page 40: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 41: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Sound stimulus produces a wave-like vibration of

basilar membrane starting from basal turn towards

apex of cochlea . It increases in amplitude as it moves

until it reaches a maximum & dies off. Sound

frequency is determined by point of maximum

amplitude. High frequency sounds cause wave with

maximum amplitude near to basal turn of cochlea.

Low frequency sound waves have their maximum

amplitude near cochlear apex.

Bekesy’s travelling wave theory

Page 42: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Georg von Bekesy

Won Nobel

prize for

his

traveling

wave

theory in

1961

Page 43: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Bekesy’s travelling wave theory

Page 44: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 45: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 46: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Theories of bone conductionCompression theory: skull vibration from sound

stimulus vibration of bony labyrinth & inner

ear fluids

Inertia theory: sound stimulus skull vibration but

ear ossicles lag behind due to inertia. Out of

phase movement of skull & ear ossicles

movement of stapes footplate vibration of

inner ear fluids

Page 47: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Theories of bone conduction

Osseo-tympanic theory: sound stimulus skull

vibration but mandible condyle lags behind due

to inertia. Out of phase movement of skull &

mandible vibration of air in external auditory

canal vibration of tympanic membrane

Tonndorf’s theory: sound stimulus skull

vibration rotational vibration of ear ossicles

movement of stapes footplate

Page 48: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 49: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Physiology of equilibrium

Balance of body during static or dynamic

positions is maintained by 4 organs:

1. Vestibular apparatus (inner ear)

2. Eye

3. Posterior column of spinal cord

4. Cerebellum

Page 50: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Vestibular apparatus

Semicircular canals

Angular acceleration & deceleration

Utricle

Horizontal linear acceleration & deceleration

Saccule

Vertical linear acceleration & deceleration

Page 51: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Orientation of semicircular canals

Page 52: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 53: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Physiology of head movementHead Movement Semicircular canal

stimulated

Yaw Lateral

Pitch Posterior + Superior

Roll Superior + Posterior

Page 54: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Nystagmus (slow component)

Page 55: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Nystagmus (fast component)

Page 56: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Semicircular canal stimulated

Nystagmus Direction

Right Lateral Right horizontal

Left Lateral Left horizontal

Right Superior Down beating, counter-clockwise

Left Superior Down beating, clockwise

Right Posterior Up beating, counter-clockwise

Left Posterior Up beating, clockwise

Page 57: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 58: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
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Page 68: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Vestibulo-ocular reflex (VOR)

Movement of head to left left horizontal canal

stimulated & right horizontal canal inhibited

To keep eyes fixed on a stationary point, both eyes

move to right side by stimulating right lateral

rectus & left medial rectus muscles

Page 69: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 70: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 71: Physiology of Hearing & Equilibrium Dr. Vishal Sharma
Page 72: Physiology of Hearing & Equilibrium Dr. Vishal Sharma

Thank You