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3/16/2010 IB Physics HL 21
Medical Physics:Hearing - IB Objectives
I.1.1 Describe the basic structure of the human ear
I.1.2 State and explain how sound pressure variations in air are changed into larger pressure variations in the cochlear fluid
I.1.3 State the range of audible frequencies experienced by a person with normal hearing
I.1.4 State and explain that a change in observed loudness is the response of the ear to a change in intensity
I.1.5 State and explain that there is a logarithmic response of the ear to intensity
3/16/2010 IB Physics HL 22
Structure of the Ear
3/16/2010 IB Physics HL 23
Structure of the Ear Outer ear:
Pinna (ear) Auditory canal Eardrum (tympanic membrane)
Middle ear: Ossicles (Hammer, anvil, and stirrup, or malleus,
incus, and stapes) Connect eardrum to cochlea
Eustachian tube Inner ear
Cochlea (snail)
3/16/2010 IB Physics HL 24
Hearing – Outer Ear
Pinna directs sound energy into auditory canal Auditory canal directs sound energy to eardrum
(tympanic membrane) Length of 2.5 cm gives resonance at 3,300 Hz
~Peak for human speech Eardrum vibrates at frequencies of sound
Area of ~60 mm2
3/16/2010 IB Physics HL 25
Hearing – Middle Ear
What is force transferred? F2 = 1.5 F1
What is pressure transferred? F2 = A2P2 = 1.5 F1 = 1.5 A1P1
P2 = 1.5 A1/A2 P1 = 30 P1
3 mm2
60 mm2
3/16/2010 IB Physics HL 26
Hearing – Middle Ear Three ossicles conduct vibration from eardrum to
cochlea Provide magnification of force of ~1.5 Provide magnification of pressure ~30 to cochlea
Cochlear oval window (fenestra ovalis) has area of ~3 mm2
Magnification of force and pressure needed to transfer pressure waves from air on eardrum to fluid in cochlea
Otherwise, most sound reflected back Pressure between outer ear and middle ear equalized
by Eustachian tube
3/16/2010 IB Physics HL 27
Hearing – Inner Ear
3/16/2010 IB Physics HL 28
Hearing – Inner Ear
Cochlear has complex structure One tube (scala vestibuli) on other side of oval
window transmits pressure wave through perilymph
Pressure wave travels to helicotrema, where scala vestibuli connects to another tube (scala tympani), and back to round window (finestra rotunda)
Pressure wave also induces waves in walls of these tubes, and in the walls of a third tube between them (scala media)
Structures in this third tube responsible for hearing
3/16/2010 IB Physics HL 29
Hearing – Inner Ear 2
Cochlear has complex structure Walls of scala media have different sizes, masses,
and tension Different resonant frequencies along tube
Fluid (mesolymph) supports hair cells and organs of corti that detect these resonances, and transmit impulses to nerves to brain
Cochlea unrolled
Oval Window
Round Window
Scala Tympani
Scala VestibuliScala Media
3/16/2010 IB Physics HL 210
Hearing – Inner Ear 3 The hair cells and the organ of Corti detect
movements in the wall (basal membrane) of the scala media Medium and high frequency sounds detected by
different regions of the cochlea Low frequencies (~200 - 1000 Hz) detected by
entire length of scala media Louder noise activates
more hair cellsMedium Freq.
ResponseHigh Freq.Response
Low Freq.Response
Cochlea Unrolled
3/16/2010 IB Physics HL 211
Human Hearing - Active Listening
Ear adjusts to hear anticipated sounds Pre-tensioning hair cells to listen for quiet sounds Eardrum tightness Support of ossicles
Ear protects itself from loud noises Reduces tight linkage between ossicles Can be too late if noise is too sudden
Ear makes its own sounds Ringing (tinnitis)
3/16/2010 IB Physics HL 212
Human Hearing - Frequency Limits
“Normal” range of human hearing given as20 Hz to 20,000 Hz Audible frequencies With age, smaller range especially at high end
Less the 20 Hz: infrasound More than 20 kHz: ultrasound
3/16/2010 IB Physics HL 213
Sound Intensity andSound Intensity Level - Decibels (dB)
Sound is longitudinal vibration in a medium Characterize intensity of sound by how much energy
it carries Per second Per square meter (area)
I (J/(s m2)) or J s-1 m-2
Because of wide range of sound levels, use unit with logarithmic scale: Intensity Level (IL)
IL (decibels) = 10 log (I/I0), where I0 = 1.0 x 10-12 W/m2
I0 is the quietest sound commonly able to be heard
3/16/2010 IB Physics HL 214
Sound Intensity andSound Intensity Level - Examples
What is IL of intensity I0
What is IL of intensity 1.0 W/m2
What is intensity of IL of 50 dB? What is intensity of IL of 36 dB?
3/16/2010 IB Physics HL 215
Perceived Sound Level -Frequency Dependence
The “threshold of hearing” is not always at I0
3/16/2010 IB Physics HL 216
Perceived Sound Level 2 -Loudness Dependence
Sounds of equal intensity are “loudest” at ~3 kHz Sounds of equal perceived loudness have same
phon values
From Everest, Frederick Alton, The Master Handbook of Acoustics
3/16/2010 IB Physics HL 217
Perceived Loudness -Loudness Dependence
We do not hear sound loudness linearly Sounds that are twice as loud have twice the sone
values Perceived
loudness(sones) showlogarithmicbehavior
From Everest, Frederick Alton, The Master Handbook of Acoustics
3/16/2010 IB Physics HL 218
Medical Physics:Hearing - IB Objectives
I.1.6 Define intensity and also intensity level (IL).
I.1.7 State the approximate magnitude of the intensity level at which discomfort is experienced by a person with normal hearing.
I.1.8 Solve problems involving intensity levels.
I.1.9 Describe the effects on hearing of short-term and long-term exposure to noise.
I.1.10 Analyze and give a simple interpretation of graphs where IL is plotted against the logarithm of frequency for normal and defective hearing.
3/16/2010 IB Physics HL 219
Effect of Distance on Sound Intensity
As a sound wave expands in space, the radius goes from R1 to R2, Intensity goes from I1 to I2
Surface area of wavefront goes from 4R12 to 4R2
2
Since energy does not change, the energy/surface area goes down
R12I1 = R2
2I2, or R12/R2
2 = I2/I1
R1
R2
3/16/2010 IB Physics HL 220
Measuring Human Hearing Hearing measured by audiologists Typically, measure threshold of hearing
Of each ear separately At a range of frequencies Report results as IL vs frequency (log)
Normal Audiogram
3/16/2010 IB Physics HL 221
Physiological Effects of Sounds
Intensity Level (dB)
Cause Effect
60 Conversation
90 Loud noise Extended exposure - hearing degraded
120 Rock concert Discomfort, possible long term effects
140 Jet engine at 25 m Pain, possible damage
160 Nearby rifle shot Eardrum rupture
~180 Explosion Death
196 Explosion Loudest sound
3/16/2010 IB Physics HL 222
Sample Problems withSound Intensity Level
A jet engine creates a sound with a 120 dB sound intensity level at 10 m. What is the sound intensity? What is the sound intensity at 65 m? How far do you have to be to hear the engine with
an intensity level of 60 dB?
3/16/2010 IB Physics HL 223
Hearing Problems Hearing problems may occur in the outer ear, middle
ear, and inner ear, or in the nerves carrying auditory information to the brain
Commonly, hearing degrades With age With exposure to noise (usually long-term)
Cilia on hair cells in cochlea break off, and are not replaced, especially for high-frequency sounds (Why?) Increasing hearing loss over time, especially at the
high frequencies
3/16/2010 IB Physics HL 224
Noise Exposure Short-term effects of noise exposure can be
Tinnitis (ringing in the ears) Reduced perceived loudness (muffled)
Long-term effects can be serious permanent degradation of hearing
Normal Audiogram
Long-term NoiseExposure
Normal 65-year old