Mechanical Properties of the Cochlea. Reading: Yost Ch. 7

Similar documents
Structure, Energy Transmission and Function. Gross Anatomy. Structure, Function & Process. External Auditory Meatus or Canal (EAM, EAC) Outer Ear

ENT 318 Artificial Organs Physiology of Ear

Auditory Physiology PSY 310 Greg Francis. Lecture 30. Organ of Corti

HST 721 Lecture 4: Mechanics, electromotility and the cochlear amplifier

Hearing Sound. The Human Auditory System. The Outer Ear. Music 170: The Ear

Music 170: The Ear. Tamara Smyth, Department of Music, University of California, San Diego (UCSD) November 17, 2016

Signals, systems, acoustics and the ear. Week 5. The peripheral auditory system: The ear as a signal processor

Auditory Physiology Richard M. Costanzo, Ph.D.

Innervation of the Cochlea. Reading: Yost Ch. 8

Auditory System. Barb Rohrer (SEI )

Intro to Audition & Hearing

Sound and its characteristics. The decibel scale. Structure and function of the ear. Békésy s theory. Molecular basis of hair cell function.

Systems Neuroscience Oct. 16, Auditory system. http:

Lecture 6 Hearing 1. Raghav Rajan Bio 354 Neurobiology 2 January 28th All lecture material from the following links unless otherwise mentioned:

What does it mean to analyze the frequency components of a sound? A spectrogram such as that shown here is the usual display of frequency components

Auditory System Feedback

SOLUTIONS Homework #3. Introduction to Engineering in Medicine and Biology ECEN 1001 Due Tues. 9/30/03

Receptors / physiology

SPHSC 462 HEARING DEVELOPMENT. Overview Review of Hearing Science Introduction

What is the effect on the hair cell if the stereocilia are bent away from the kinocilium?

Can You Hear Me Now?

Sound. Audition. Physics of Sound. Properties of sound. Perception of sound works the same way as light.

Audition. Sound. Physics of Sound. Perception of sound works the same way as light.

Acoustics Research Institute

Chapter 3: Anatomy and physiology of the sensory auditory mechanism

Hearing. istockphoto/thinkstock

Cochlear anatomy, function and pathology I. Professor Dave Furness Keele University

MECHANISM OF HEARING

Chapter 17, Part 2! The Special Senses! Hearing and Equilibrium!

Chapter 17, Part 2! Chapter 17 Part 2 Special Senses! The Special Senses! Hearing and Equilibrium!

HEARING AND PSYCHOACOUSTICS

Acoustics, signals & systems for audiology. Psychoacoustics of hearing impairment

Auditory Physiology PSY 310 Greg Francis. Lecture 29. Hearing

PSY 310: Sensory and Perceptual Processes 1

Chapter 11: Sound, The Auditory System, and Pitch Perception

Sound and Hearing. Decibels. Frequency Coding & Localization 1. Everything is vibration. The universe is made of waves.

The Structure and Function of the Auditory Nerve

The frequency analysis of the cochlea a review of Nobili et al (1998) and Ruggero et al (1992)

A truly remarkable aspect of human hearing is the vast

Printable version - Hearing - OpenLearn - The Open University

Improving the diagnostic power of otoacoustic emissions. Arturo Moleti Physics Department University of Roma Tor Vergata

Processing of sounds in the inner ear

Music and Hearing in the Older Population: an Audiologist's Perspective

Modelling the micromechanics of the cochlea in Femlab

AUDL GS08/GAV1 Signals, systems, acoustics and the ear. Pitch & Binaural listening

Hearing: Physiology and Psychoacoustics

College of Medicine Dept. of Medical physics Physics of ear and hearing /CH

Required Slide. Session Objectives

Sound Waves. Sensation and Perception. Sound Waves. Sound Waves. Sound Waves

Human Acoustic Processing

Anatomy and Physiology of Hearing

Deafness and hearing impairment

Nature Biotechnology: doi: /nbt Supplementary Figure 1. Analysis of hair bundle morphology in Ush1c c.216g>a mice at P18 by SEM.

Hearing and Balance 1

Hearing. By: Jimmy, Dana, and Karissa

PSY 214 Lecture # (11/9/2011) (Sound, Auditory & Speech Perception) Dr. Achtman PSY 214

Spectrograms (revisited)

Modeling of Mechanoelectrical Transduction of Hair Cells to Action Potentials in the Auditory Nerve

Hearing. PSYCHOLOGY (8th Edition, in Modules) David Myers. Module 14. Hearing. Hearing

Consequences of Location-Dependent Organ of Corti Micro-Mechanics

BCS 221: Auditory Perception BCS 521 & PSY 221

An active cochlear model showing sharp tuning and high sensitivity

HEARING. Structure and Function

Welcome to Cochlear Dead Regions and Implications for Fittings. Presenter: Audiologist, Speaker, Author. IHS Organizers: Housekeeping

Chapter 1: Introduction to digital audio

to vibrate the fluid. The ossicles amplify the pressure. The surface area of the oval window is

Unit VIII Problem 9 Physiology: Hearing

Chapter 3. Sounds, Signals, and Studio Acoustics

FIFTH INTERNATIONAL CONGRESS ON SOUND AND VIBRATION DECEMBER 15-18, 1997 ADELAIDE, SOUTH AUSTRALIA. Invited Paper LINEAR RESPONSE OF THE COCHLEA

SPECIAL SENSES: THE AUDITORY SYSTEM

Rods vs Cones 3/10/2014. Example 1: Light Sensitive Visual Receptors. Turning Light Waves Into Electrical Messages (Transduction)

9.01 Introduction to Neuroscience Fall 2007

What you re in for. Who are cochlear implants for? The bottom line. Speech processing schemes for

Auditory Periphery! external middle inner. stapes movement initiates a pressure wave in cochlear fluid

Chapter Fourteen. The Hearing Mechanism. 1. Introduction.

Essential feature. Who are cochlear implants for? People with little or no hearing. substitute for faulty or missing inner hair

EMANATIONS FROM RESIDUUM OSCILLATIONS IN HUMAN AUDITORY SYSTEM

Auditory-based Automatic Speech Recognition

AUDL GS08 and GAV1: 2013 Final exam page 1/13. You must complete all sections. Label all graphs. Show your work!

Week 5. Fall 2016 Part 2: Structure and Function of Auditory System 1

Chapter 13 Physics of the Ear and Hearing

Before we talk about the auditory system we will talk about the sound and waves

Representation of sound in the auditory nerve

PSY 215 Lecture 10 Topic: Hearing Chapter 7, pages

Academic and Research Staff Professor Dennis M. Freeman, Dr. Alexander Aranyosi, Dr. Stanley Hong

Lecture 3: Perception

Hearing. Juan P Bello

Topic 4. Pitch & Frequency. (Some slides are adapted from Zhiyao Duan s course slides on Computer Audition and Its Applications in Music)

Educational Module Tympanometry. Germany D Germering

Compression in Hearing Aids

external middle inner

Topic 4. Pitch & Frequency

Assessment of crossed auditory paths using Distortion-Product Otoacoustic Emissions

Cochlear anatomy, function and pathology II. Professor Dave Furness Keele University

Hearing I: Sound & The Ear

Ear. Utricle & saccule in the vestibule Connected to each other and to the endolymphatic sac by a utriculosaccular duct

L2: Speech production and perception Anatomy of the speech organs Models of speech production Anatomy of the ear Auditory psychophysics

The Ear. The ear can be divided into three major parts: the outer ear, the middle ear and the inner ear.

Digital Speech and Audio Processing Spring

Who are cochlear implants for?

Transcription:

Mechanical Properties of the Cochlea CF Reading: Yost Ch. 7

The Cochlea Inner ear contains auditory and vestibular sensory organs. Cochlea is a coiled tri-partite tube about 35 mm long. Basilar membrane, supporting the Organ of Corti, runs along entire length of cochlea. Its mechanical properties change as a function of distance from the stapes: designed to analyze frequency components in complex sounds. Hair cells receptors in Organ of Corti of two types: inner (single row) and outer (3/4 rows) Stereocilia are rigid rods interconnected on their flanks, and at their tips. Tip links critical to transduction.

Traveling Wave Stapes vibration generates pressure waves in fluids of cochlea. Pressure waves generate vibrations of the basilar membrane that propagate from base to apex along the basilar membrane as a traveling wave (von Békesy 1961) BM vibrates at the same frequency as the simple sound stimulus wherever the basilar membrane is set in motion by the TW. Amplitude of the TW differs at different locations, depending on frequency and amplitude (acoustic energy) of the stimulus.

Traveling Wave Motion The vibratory motion of the basilar membrane is a traveling wave. A traveling wave moves longitudinally from one place (stapes) to another place (helicotrema) (like that in a rope with the far end free) Top (a): snapshot of basilar membrane model showing instantaneous vibration pattern and shape of traveling wave (as seen from the side). Bottom (b): More accurate view of pattern, with membrane attached at sides. Note that different regions of membrane are out of phase, with a greater phase difference ahead of the peak of the wavefront (apical) than behind it (basal). Base Apex

Envelope of Traveling Wave For a given traveling wave, basilar membrane displacement changes as a function of distance from apex to base. If a line is drawn through the points of maximum displacement for a specific traveling wave, then the resulting curve is called the envelope of the traveling wave. Numbered curves: freeze-frames of TW for a sustained pure tone stimulus taken at different instants in time. Different locations along the membrane displaced in opposite directions (called a local phase difference). For pure tone stimulus, the TW envelope shows a single maximum of displacement.

Traveling wave peak shifts from base to apex as stimulus frequency is varied from high to low (von Bekesy 1947). TW for low frequencies stretches over a long distance, can vibrate nearly entire basilar membrane if sound sufficiently intense. TW for high frequencies more confined, only stimulates the base. Place Theory

Why do Sounds Generate a TW? Each point along the basilar membrane that is set in motion vibrates at the same frequency as the stimulus. However, different frequencies will cause maximum vibration amplitude at different points and times along the membrane. A number of factors vary along the length of the cochlea. In particular, moving from base to apex: BM width increases (higher mass) BM becomes thinner (less stiffness) Stereocilia get longer (higher mass, less stiffness). These changes reduce the resonant frequency of the basilar membrane with distance from the stapes (F r a s/m), and thus increase time to peak response.

Complex sounds create complex traveling wave patterns, with multiple vibration maxima. Pattern of excitation provides information about Frequency Amplitude Temporal variation Complex Sounds Note that due to the traveling wave, low frequency components of a sound are transduced after high frequency components... The TW introduces temporal distortions (absolute time and relative phase delays)! Envelope of basilar membrane displacement to 50 Hz or 100 Hz alone, and combined as F 0 and F 1 of a harmonic series.

Mechanical Tuning in Organ of Corti Mechanical tuning of any point along BM resembles bandpass filter, with a steep high-frequency roll-off, and a shallow lowfrequency roll-off. Mechanical tuning curves Characteristic frequency (CF): Frequency at which the sound level reaches a minimum to obtain a criterion displacement for that position on the BM Thus, the organ of Corti topographically decomposes the spectrum of the sound with frequency-selective bandpass filters (channels). CF Iso-sensitivity curve of basilar membrane plotted as equal-displacement function re 19 Ångstroms ( 1.9 x 10-8 cm) CF = 8350 Hz.

Basilar Membrane Nonlinearity The higher the stimulus level, the greater the amplitude of basilar membrane displacement. Displacement of BM is not linear as a function of stimulus level near the peak of the TW. Consequence: Near CF, range of BM motion is less than the range of sound levels, i.e. the dynamic range shows compressive non-linearity. Compressive nonlinearity generates distortion products (e.g., harmonics, difference tones). Input-output ( transfer ) function: BM velocity vs sound level. (CF =9000 Hz)

Mechanical Excitation of Hair Cells TM OHCs Traveling wave causes up-and-down motion of basilar membrane and tectorial membrane (at same frequency as stimulus). IHCs Displacement sets up transverse shearing force that deflects hair cell stereocilia. Kiang 1984 BM after Wada 2002

Mechanical Excitation: Outer Hair Cells Tips of OHC stereocilia are embedded in tectorial membrane. BM pivots around inner pillar cell attachment to spiral lamina when stimulated. Stereocilia deflected by mechanical shearing: tectorial membrane pushes and pulls as hair cells move back and forth. Geisler 1998

Mechanical Excitation: Inner Hair Cells Model of putative fluid shearing mechanism of stereocilia bundle deflection and excitation in IHCs. Geisler 1998

Summary Excitation of inner ear gives rise to traveling wave along the basilar membrane, due to longitudinal changes in the basilar membrane (principally, compliance stiffness) Changes in sound frequency shift the location of the traveling wave peak along the basilar membrane, creating a place code for frequency (tonotopy). Hair cells are stimulated by basilar membrane traveling wave(s): they are mechanically tuned to a single CF according to their location on the BM; and the amplitude of their vibration is related to stimulus level. CF