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 1 IB Physics HL 2 Structure of the Ear 3/16/2010 2 IB Physics HL 2 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 3 IB Physics HL 2 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 2 Area of ~60 mm 3/16/2010 4 IB Physics HL 2 Hearing – Middle Ear 3 mm2 60 mm2 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 3/16/2010 5 IB Physics HL 2 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 6 IB Physics HL 2 Hearing – Inner Ear 3/16/2010 7 IB Physics HL 2 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 8 IB Physics HL 2 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 Scala Vestibuli Scala Media Oval Window Round Window Scala Tympani 3/16/2010 9 IB Physics HL 2 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 High Freq. Medium Freq. Response Response more hair cells Cochlea Unrolled Low Freq. Response 3/16/2010 10 IB Physics HL 2 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 11 IB Physics HL 2 Human Hearing - Frequency Limits “Normal” range of human hearing given as 20 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 12 IB Physics HL 2 Sound Intensity and Sound 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) 2 -1 m-2 I (J/(s m )) or J s 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 13 IB Physics HL 2 Sound Intensity and Sound 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 14 IB Physics HL 2 Perceived Sound Level Frequency Dependence The “threshold of hearing” is not always at I0 3/16/2010 15 IB Physics HL 2 Perceived Sound Level 2 Loudness Dependence Sounds of equal intensity are “loudest” at ~3 kHz Sounds of equal perceived loudness have same phon values 3/16/2010 From Everest, Frederick Alton, The Master Handbook of Acoustics 16 IB Physics HL 2 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) show logarithmic behavior 3/16/2010 From Everest, Frederick Alton, The Master Handbook of Acoustics 17 IB Physics HL 2 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 18 IB Physics HL 2 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 4R22 Since energy does not change, the energy/surface area goes down R12I1 = R22I2, or R12/R22 = I2/I1 R1 R2 3/16/2010 19 IB Physics HL 2 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 20 IB Physics HL 2 Physiological Effects of Sounds Intensity Cause Level (dB) 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 21 IB Physics HL 2 Sample Problems with Sound 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 22 IB Physics HL 2 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 23 IB Physics HL 2 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 Long-term Noise Exposure Normal 65-year old Normal Audiogram 3/16/2010 24 IB Physics HL 2