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9/21/2020 1 From Sound to Action Potentials - a Tour of the Inner Ear William E. Brownell Professor Emeritus, Dpt Oto–H&N Surgery ARO seminar series, September 17, 2020 [email protected] ACTION POTENTIALS in the auditory brainstem von Gersdorff & Borst, 2002 Brownell, 1975 Goldberg & Brownell, 1973 Joris et al, 1994 Synaptic Ribbons in Sensory Cells Moser et al. Physiol Rev. 2020 1 2 3

Brownell Seminar Series Presentation...spikes (0 < p< 2π) relative to the signal. The sum of these vectors, normalized by the number of spikes, gives the vector strength r. With perfect

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  • 9/21/2020

    1

    From Soundto Action Potentials

    - a Tour of the Inner Ear

    William E. BrownellProfessor Emeritus, Dpt Oto–H&N SurgeryARO seminar series, September 17, 2020

    [email protected]

    ACTION POTENTIALS in the auditory brainstem

    von Gersdorff & Borst, 2002

    Brownell, 1975

    Goldberg & Brownell, 1973

    Joris et al, 1994

    Synaptic Ribbons in 

    Sensory Cells

    Moser et al. Physiol Rev. 2020

    1

    2

    3

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    2

    Sound enters the human ear

    stapes

    Human cochlea

    scala tympani

    basilar membrane

    organ of Corti

    scala media

    scala vestibuli

    tectorial membrane

    inner hair cells

    outer hair cells

    basilar membrane

    The cochlea and the organ of Corti

    Anatomy of a Hair Cell

    4

    5

    6

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    Mechanoelectrical Transduction

    Finding the Silent Current

    A standing current that powers:

    1. mechanotransduction2. cochlear  amplifier

    Organ ofCorti

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    8

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    1966 ‐ Heinrich Spoendlin

    discovers that up to 95 percent of auditory nerve fibers terminate on the inner hair cells

    Acoustic world enters via  SGC1

    Spoendlin, Fortschr Hals Nasen Ohrenheilkd 1966

    SGC1: type 1 spiral ganglion cells

    SGC2

    The travelling wave

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    11

    12

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    Electromotility& the Cochlear Amplifier

    200 msec pulses from a holding potential of –60 mV. Initial pulse is hyperpolarizing and each successive pulse +10 MV from that. 

    OHC displacements (ΔL)

    -200 -150 -100 -50 0 50-2.0

    -1.5

    -1.0

    -0.5

    0.0

    0.5

    L (

    m)

    V (mV)

    Data of Santos-Sacchi, 1992

    1. ΔL  f (current)

    2. ΔL  f (calcium)

    3. ΔL  f (ATP)

    4. ΔL = f (prestin &small anions)     

    5. ΔL = f (voltage)

    The OHC generates force 

    at> 80 kHz

    Frank et al., 1999

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    14

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    The Swing A Passive Filter

    The Swinger An Active Filter

    Viscosity limits the frequency of cochlear vibrations

    Frequencyincrease

    fkm

    Compton’s Interactive Encyclopedia, 1997

    3000 Swings

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    Normal versus impaired cochlea

    Normal system Damaged system

    Inner hair cells

    Outerhair cells

    0

    20

    40

    60

    80

    0 20 40 60 80 100 120

    Sound Pressure Level (dB)

    Velo

    city

    (dB

    re 1

    mic

    ron/

    sec)

    Live

    Post‐mortem

    (Ruggero et al., 1997)

    40 dB

    ~10 dB

    4:1 compression

    Damage to the outer hair cells

    Aspirin Ototoxicity

    Male (60 yrs) with hearing loss

    Myer & Bernstein, 1965

    Salicylate blocks otoacoustic emissions ‐ McFaddden & Plattsmier, 1984

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    Aspirin OtotoxicitySalicylate application blocks OHC electromotility

    Electromotile mechanismis in the plasma membrane

    OHC is a hydrostat with unusual cytoarchitectonics

    Brownell et al., 1985 Brownell, 1990

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    Dieler et al., 1991

    Plasma membrane folding

    Holley et al., 1992

    •Actin ‐ circumferential•Spectrin ‐ longitundinal•Pillars ‐ radial

    The OrthotropicCortical Lattice

    The OHC lateral wall: a trilaminate structure

    Brownell and Popel, 1998

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    Electron tomography update of lateral wall

    Triffo et al Front Cell Neuro, 2019

    OHC electromotility – voltage induced change in membrane curvature

    Converse flexoelectricity

    Petrov and Sachs, Phys Rev E, 2002

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    Direct flexoelectricity

    Dong et al., 2002

    Non mammals have Cochlear Amplifiers but NO OHCs

    They do have otoacoustic emissionsTheir hair cells do not have somatic motilityAmplifier is postulated to originate in stereociliaA form of electromotility/adaptation occurs in hair cell stereocilia bundles

    Stereocilia as flexoelectric motorsfrom: Breneman, Brownell & Rabbitt ‐ 2009

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    Predicts stereocilia length

    Electromechanics in membrane tethers

    Brownell et al., 2010

    Flexoelectric model compatible with optical tweezers 

    results

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    Add an acsessory mass and explicitly include cationic influx through MET

    Deng et al.,  Mech Physics Solids. 2019

    Selectivity and critical limit cycle

    Convergence to a critical limit cycle

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    Benefits to hearing

    Hudspeth et al, 2010

    Trilaminate Structures

    40

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    Prestin

    AA

    LL

    F

    Cluster 1 Cluster 2

    0.998

    1.000

    1.002

    1.004

    1.006

    1.008

    -0.2 0.0 0.2

    C()/C(0)

    (Volts)

    0.4

    0.6

    0.8

    1

    1.2

    -0.2 0 0.2

    C()/C p

    eak

    OHC HEK

    Prestin associated charge movement

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    Cholesterol level shifts Vpkc in OHCs

    Cholesterol in prestin transfected HEK cells

    Phase locking & vector strength

    Goldberg and Brown, 1969

    Vector strength: Each spike is represented by a vector of unit length and direction equal to the phase, p, of the spikes (0 

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    Outer Hair Cellsare surrounded by fluid

    Wiggins & Phillips, 2005 

    Bilayer‐inclusion model

    Na V Channel , Payandeh et al, 2011 Prestin, Gorbunov et al, 2014

    Organ ofCorti

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    Inner Ear Mechanoreceptor OrgansVestibular system > 400 million years old 0‐102 Hz

    Mammalian Cochlea ~ 200 million years old, 101‐105 Hz

    Outer hair cell electromotility

    200 msec pulses from a holding potential of –60 mV. Initial pulse is hyperpolarizing and each successive pulse +10 MV from that.

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    Mechanoelectrical Transduction

    Harnessing membrane EMF by stereocilia

    100 nm

    Potential impact on mechanics

    Hudspeth et al, 2010

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