hearing balance

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    Physiology and Biophysics of

    Auditory and Vestibular function

    Dr. Charles CapadayProfessor & DirectorBrain and Movement Laboratory

    CRULRG, F-65002601 de la Canardiere, Qubec City (QC),

    G1J 2G3, Canadahttp://www.BrainAndMovementLab.org/

    http://www.brainandmovementlab.org/http://www.brainandmovementlab.org/http://www.brainandmovementlab.org/http://www.brainandmovementlab.org/http://www.brainandmovementlab.org/
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    The sensitivity of the ear is remarkable.

    Some facts:At 2-3 kHz the threshold of hearing intensity is about 10-16W/cm2.

    This corresponds to a pressure variation of 2.9 x 10-4dyn/cm2, the

    background atmospheric pressure is 1.013 x106dyn/cm2(101.3 kPa).

    Random pressure variations due to thermal motion of air molecules is0.5 x 10-4dyn/cm2 ! The sensitivity of the ear is thus close to thetheoretical limit, being just above the thermal noise level.

    At the threshold power level (10-16W/cm2) the displacement of the air

    molecules is less than the size of the molecules themselves!

    1 1 2

    1 1 2

    2

    22

    4

    ( )

    It p v p v

    Ii p v p v

    From which it is readily apparent that only 0.1% of the soundenergy enters the water. Water is a very

    good sound barrier.

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    The sensitivity of the ear is partly due to its mechanicalconstruction which amplifies sound pressure

    The area of the eardrum is 30times larger than that of theoval window. So byArchimides principle

    The ossicles act as a leversystem with a mechanicaladvantage of about 2.

    The ear canal has a resonantfrequency circa 3 kHz,

    amplifying the pressure by afactor of about 2.

    Thus, 2 x 30 x 2 =120.However,

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    What we will explain

    Sensitivity curve of human ear Sound Localization

    -4

    sin

    lt= , where v is sound velocity

    v

    0.085 m. . 2.5 x 10 0.25

    340m/s

    In fact time differences of the order of 30 s can be detected,corresponding to an angle of about 3 deg.

    l d

    e g t s ms

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    Why primary afferent fibre firing rate is nonlinearlyrelated to stimulus intensity (but not always)

    x 0 0.10 1000

    y1 1 y2 800

    y3 x( ) x0.3

    0 500 10000

    500

    1000

    Y-axis in Linear Scale

    y1

    y2

    x

    0 500 10000.01

    0.1

    1

    10100

    1 103

    1 104

    Y-axis in Log Scale

    y1

    y2

    x

    0 200 400 600 800 10000

    5

    10

    Power Function with Exponent = 0.3

    y3 x( )

    x

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    The mammalian central auditory pathways (fordummies version).

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    A1 is tonotopically organized

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    Neural Mechanisms of sound localization

    The medial superiorolive transforms atime code into a

    place code.

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    The Barn Owls Story

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    A measured behaviour and its underlyingneural systems

    See, T. Carew. Behavioural Neurobiology. Sinauer Associates, 2000.