Color Atlas of Physiology 2003 thieme
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A. Visual field (right eye) |
B. Visual pathway and visual field deficits |
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Temple |
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Visual field |
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Blind spot |
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90° |
60° |
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104° |
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C. Successive color contrast |
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Optic nerve |
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Explained on p. 354 |
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Optic chiasm |
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Optic tract |
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Superior |
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colliculi |
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Lateral |
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geniculate |
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body |
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Optic radiation |
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Secondary |
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visual cortex |
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(V2 , etc.) |
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Primary |
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visual cortex (V1 , etc.) |
Plate 12.25 Visual Field, Visual Pathway
Color, high-resolution stationary shapes, movement, and stereoscopic depth are processed in some subcortical visual pathways, and from V1 onward in separate information channels. These individual aspects must be integrated to achieve visual perception. In diurnally active primates like humans, over half of the cortex is involved in processing visual information. On a simplified scale, the parietal cortex analyzes the “where” and involves motor systems, and the temporal cortex takes care of the “what” of visual input comparing it with memory.
Axons of the optic tract (especially those of M and γ cells) also project to subcortical regions of the brain such as the pretectal region, which regulates the diameter of the pupils (see below); the superior colliculi (!B), which are involved in oculomotor function (!p. 360);
the hypothalamus, which is responsible for circadian rhythms (!p. 334).
The pupillary reflex is induced by sudden exposure of the retina to light (!p. 350). The signal is relayed to the pretectal region; from here, a parasympathetic signal flows via the Edinger–Westphal nucleus, the ciliary ganglion and the oculomotor nerve, and induces narrowing of the pupils (miosis) within less than 1 s. Since both pupils respond simultaneously even if the light stimulus is unilateral, this is called a consensual light response. Meiosis also occurs when the eyes adjust for near vision (near-vision response !p. 360).
The corneal reflex protects the eye. An object touching the cornea (afferent: trigeminal
nerve) or approaching the eye (afferent: optic 359 nerve) results in reflex closure of the eyelids.
Despopoulos, Color Atlas of Physiology © 2003 Thieme
All rights reserved. Usage subject to terms and conditions of license.
Eye Movements, Stereoscopic Vision,
Depth Perception
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Conjugated movement of the eyes occurs when |
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the external eye muscles move the eyes in the |
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same direction (e.g., from left to right), |
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Senses |
whereas vergence movement is characterized |
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by opposing (divergent or convergent) eye |
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when gazing into the distance. Fixation of the |
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and |
movement. The axes of the eyes are parallel |
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gaze on a nearby object results in convergence |
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System |
of the visual axes. In addition, the pupil con- |
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tracts (to increase the depth of focus) and ac- |
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commodation of the lens occurs (!p. 346). |
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Nervous |
The three reactions are called near-vision re- |
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sponse or convergence response. |
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Strabismus. A greater power of accommodation for |
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near vision is required in hyperopia than in normal vi- |
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sion. Since accommodation is always linked with a |
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convergence impulse, hyperopia is often associated |
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with squinting. If the visual axes wander too far |
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apart, vision in one eye will be suppressed to avoid |
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double vision (diplopia). This type of visual impair- |
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ment, called strabismic amblyopia, can be either tem- |
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porary or chronic. |
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Saccades. When scanning the visual field, the |
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eyes make jerky movements when changing |
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the point of fixation, e.g., when scanning a line |
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of print. These quick movements that last |
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10–80 ms are called saccades. Displacement of |
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the image is centrally suppressed during the |
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eye due to saccadic suppression. A person look- |
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ing at both of his or her eyes alternately in a |
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mirror cannot perceive the movement of his or |
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her own eyes, but an independent observer |
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can. The small, darting saccades function to |
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keep an object in focus. |
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Objects entering the field of vision are re- |
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flexively imaged |
in the fovea centralis |
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(!p. 348). Slow |
pursuit movements of the |
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eyes function to maintain the gaze on moving |
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objects. Nystagmus is characterized by a com- |
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bination of these slow and rapid (saccade-like) |
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opposing eye movements. The direction of |
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nystagmus (right or left) is classified according |
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to the type of rapid phase, e.g., secondary nys- |
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tagmus (!p. 342). Optokinetic nystagmus oc- |
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curs when viewing an object passing across |
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the field of vision, e.g., when looking at a tree |
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360 |
from inside a moving train. Once the eyes have |
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returned to the normal position (return sac- |
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cade), a new object can be brought into focus. Damage to the cerebellum or organ of balance (!p. 342) can result in pathological nystagmus.
The brain stem is the main center responsible for programming of eye movements. Rapid horizontal (conjugated) movements such as saccades and rapid nystagmus movement are programmed in the pons, whereas vertical and torsion movements are programmed in the mesencephalon. The cerebellum provides the necessary fine tuning (!p. 326). Neurons in the region of the Edinger–Westphal nucleus are responsible for vergence movements.
In near vision, depth vision and three-di- mensional vision are primarily achieved through the coordinated efforts of both eyes and are therefore limited to the binocular field of vision (!A). If both eyes focus on point A (!B), an image of the fixation point is projected on both foveae (AL, AR), i.e., on the corresponding areas of the retina. The same applies for points B and C (!B) since they both lie on a circle that intersects fixation point A and nodal points N (!p. 347 B) of the two eyes (Vieth– Müller horopter). If there were an imaginary middle eye in which the two retinal regions (in the cortex) precisely overlapped, the retinal sites would correspond to a central point AC ! AL + AR (!C). Assuming there is a point D outside the horopter (!C, left), the middle eye would see a double image (D!, D ) instead of point D, where D! is from the left eye (DL). If D and A are not too far apart, central processing of the double image creates the perception that D is located behind D, i.e., depth perception occurs. A similar effect occurs when a point E (!C, right) is closer than A; in this case, the E! image will arise in the right eye (E!R) and E will be perceived as being closer.
Depth perception from a distance. When viewing objects from great distances or with only one eye, contour overlap, haze, shadows, size differences, etc. are cues for depth perception (!D). A nearby object moves across the field of vision more quickly than a distant object, e.g., in the case of the sign compared to the wall in plate D). In addition, the moon appears to migrate with the moving car, while the mountains disappear from sight.
Despopoulos, Color Atlas of Physiology © 2003 Thieme
All rights reserved. Usage subject to terms and conditions of license.
A. Binocular visual field
Binocular |
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visual field |
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75° |
45° |
15° |
Left |
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Right |
visual field |
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visual field |
B. Horopter |
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A |
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Perception |
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B |
C |
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K |
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K |
Depth |
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CL |
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BR |
Movements, |
AL |
BL |
CR |
AR |
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Corresponding areas |
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Eye |
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on retina |
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C. Three-dimensional vision (binocular vision)
D’ D D’’
More distant
A A
Closer
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Plate 12.26
AL |
DL |
AR |
EL |
AL |
ER |
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DR |
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AR |
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D’’R AMD’L |
Imaginary middle eye |
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E’’L AME’R |
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D. Cues for depth vision
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Shadow |
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Size |
Contour |
Haze |
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differences |
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Photo: A. Rothenburger
U L M |
L M |
Do not lean out |
Do not lean out |
361 |
Direction of train movement
Despopoulos, Color Atlas of Physiology © 2003 Thieme
All rights reserved. Usage subject to terms and conditions of license.
Physical Principles of Sound—Sound
Stimulus and Perception
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Sound waves are the adequate stimulus for the |
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organ of hearing. They arise from a sound |
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source such as a gong (!A1) and are con- |
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ducted in gases, liquids, and solids. The air is |
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the main carrier of sound. |
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The air pressure rises and falls rhythmically at the |
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and |
sound source. These pressure waves (sound waves) |
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travel at a characteristic sound velocity (c) in differ- |
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ent materials, e.g., at 332 m/s in air of 0 !C. A graphic |
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recording of sound waves (!A1) will produce |
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waveform curves. The wavelength (λ) is the dis- |
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tance between the top of one wave and the identical |
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Nervous |
phase of the succeeding one, and the maximum de- |
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will lower (raise) the tone, whereas a fall (rise) in |
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viation of pressure from baseline is the amplitude |
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(a) (!A1). Enlargement (reduction) of wavelength |
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amplitude will produce a quieter |
(louder) tone |
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(!A1). The pitch of a tone is defined by its |
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frequency (f), i.e., the number of sound pressure |
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oscillations per unit time. Frequency is measured in |
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hertz (Hz = s– 1). Frequency, wavelength and the |
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sound velocity are related: |
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f (Hz) ! λ (m) = c (m ! s– 1). |
[12.1] |
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A pure tone has a simple sinus waveform. The tones |
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emanating from most sound sources (e.g., musical |
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instrument, voice) are mixtures of different frequen- |
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cies and amplitudes that result in complex periodic |
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vibrations referred to as sound (!A2). The fun- |
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damental (lowest) tone in the complex determines the pitch of the sound, and the higher ones determine its timbre (overtones). An a1 (440 Hz) sung by a tenor or played on a harp has a different sound than one produced on an organ or piano. The overlap of two very similar tones produces a distinct effect characterized by a beat tone of a much lower frequency (!A3, blue/red).
Audibility limits. Healthy young persons can hear sounds ranging in frequency from 16 to 20 000 Hz. The upper limit of audibility can drop to 5000 Hz due to aging (presbycusis). At 1000 Hz, the absolute auditory threshold or lowest sound pressure perceived as sound is 3 · 10– 5 Pa. The threshold of sound is frequency-dependent (!B, green curve). The threshold of hearing for a tone rises tremendously when other tones are heard simultaneously. This phenomenon called masking is the reason why it is so difficult to carry on a conversation against loud background noise.
362The ear is overwhelmed by sound pressures over 60 Pa, which corresponds to 2 · 106 times
the sound pressure of the limit of audibility at
1000 Hz. Sounds above this level induce the sensation of pain (!B, red curve).
For practical reasons, the decibel (dB) is used as a logarithmic measure of the sound pressure level (SPL). Given an arbitrary reference sound pressure of po = 2 · 10– 5 Pa, the sound pressure level (SPL) can be calculated as follows:
SPL (dB) = 20 · log (px/po) |
[12.2] |
where px is the actual sound pressure. A tenfold increase in the sound pressure therefore means that the SPL rises by 20 dB.
The sound intensity (I) is the amount of sound energy passing through a given unit of area per unit of time (W · m2). The sound intensity is proportional to the square of px. Therefore, dB values cannot be calculated on a simple linear basis. If, for example, two loudspeakers produce 70 dB each (px = 6.3 · 10-2 Pa), they do not produce 140 dB together, but a mere 73 dB because px only increases by a factor of !"2 when the intensity level doubles. Thus, !"2 · 6.3 · 10–2 Pa has to be inserted for px into Eq. 12.2.
Sound waves with different frequencies but equal sound pressures are not subjectively perceived as equally loud. A 63 Hz tone is only perceived to be as loud as a 20 dB/1000 Hz reference tone if the sound pressure of the 63 Hz tone is 30-fold higher (+ 29 dB). In this case, the sound pressure level of the reference tone (20 dB/1000 Hz) gives the loudness level of the 63 Hz tone in phon (20 phon) as at a frequency of 1000 Hz, the phon scale is numerically equals the dB SPL scale (!B). Equal loudness contours or isophones can be obtained by plotting the subjective values of equal loudness for test frequencies over the whole audible range (!B, blue curves). The absolute auditory threshold is also an isophone (4 phons; !B, green curve). Human hearing is most sensitive in the 2000–5000 Hz range (!B).
Note: Another unit is used to describe how a tone of constant frequency is subjectively perceived as louder or less loud. Sone is the unit of this type of loudness, where 1 sone = 40 phons at 1000 Hz. 2 sones equal twice the reference loudness, and 0.5 sone is 1/2 the reference loudness.
The auditory area in diagram B is limited by the highest and lowest audible frequencies on the one side, and by isophones of the thresholds of hearing and pain on the other. The green area in plate B represents the range of frequencies and intensities required for comprehension of ordinary speech (!B).
Despopoulos, Color Atlas of Physiology © 2003 Thieme
All rights reserved. Usage subject to terms and conditions of license.
A. Wavelength, wave amplitude and wave types
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Pure tone |
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Wavelength |
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Thresholds |
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pressure |
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λ |
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λ |
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Ampli- |
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0 |
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tude (a) |
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Fundamental and overtones |
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and |
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Change in frequency |
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Higher pitch |
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λ |
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Physics |
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Wavelength |
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Noise |
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Sound |
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12.27 |
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Lower pitch |
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λ |
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Change in intensity |
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Plate |
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Quieter |
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Louder |
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Beat tone |
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Ampli- |
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tude |
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B. Sound pressure, sound pressure level and loudness level |
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2.102 |
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140 |
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Phon |
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Pain threshold |
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2.101 |
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130 |
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130 phon |
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120 |
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Pneumatic drill |
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2 |
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100 |
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100 |
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120 phon |
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2.10–1 |
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Loudness level (phon) |
Heavy traffic |
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pressure level (dB SPL) |
80 |
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80 |
70–90 phon |
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2.10–2 |
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Principal |
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Normal |
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60 |
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conversational |
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conversation |
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pressure (Pa) |
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range |
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50–70 phon |
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2.10–3 |
40 |
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40 |
Whisper |
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20–40 phon |
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2.10–4 |
20 |
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Absolute |
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Sound |
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Sound |
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2.10–5 |
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4 phon |
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31.5 |
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16000 |
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Frequency (Hz) |
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363 |
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Phon = dB at 1000Hz |
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Despopoulos, Color Atlas of Physiology © 2003 Thieme
All rights reserved. Usage subject to terms and conditions of license.
Conduction of Sound, Sound Sensors
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Sound waves are transmitted to the organ of |
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hearing via the external ear and the auditory |
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canal, which terminates at the tympanic mem- |
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brane or eardrum. The sound waves are con- |
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Senses |
ducted through the air (air conduction) and set |
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the eardrum in vibration. These are trans- |
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cavity (middle ear) to the membrane of the oval |
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mitted via the auditory ossicles of the tympanic |
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window (!A 1,2), where the internal or inner |
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ear (labyrinth) begins. |
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In the middle ear, the malleus, incus and |
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stapes conduct the vibrations of the tympanic |
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membrane to the oval window. Their job is to |
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sistance in fluid with as little loss of energy as |
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conduct the sound from the low wave re- |
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sistance/impedance in air to the high re- |
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possible. This impedance transformation oc- |
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curs at f !2400 Hz and is based on a 22-fold |
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pressure amplification (tympanic membrane |
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area/oval window area is 17 : 1, and leverage |
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arm action of the auditory ossicles amplifies |
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force by a factor of 1.3). Impairment of im- |
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pedance transforming capacity due, e.g., to de- |
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struction of the ossicles, causes roughly 20 dB |
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of hearing loss (conduction deafness). |
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Muscles of the middle ear. The middle ear contains |
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two small muscles—the tensor tympani (insertion: |
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manubrium of malleus) and the stapedius (insertion: |
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stapes)—that can slightly attenuate low-frequency |
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sound. The main functions of the inner ear muscles |
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are to maintain a constant sound intensity level, pro- |
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tect the ear from loud sounds, and to reduce dis- |
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tracting noises produced by the listener. |
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Bone conduction. Sound sets the skull in vibra- |
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tion, and these bone-borne vibrations are conducted |
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directly to the cochlea. Bone conduction is fairly in- |
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significant for physiological function, but is useful for |
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testing the hearing. In Weber’s test, a vibrating |
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tuning fork (a1) is placed in the middle of the head. A |
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person with normal hearing can determine the loca- |
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tion of the tuning fork because of the symmetrical |
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conduction of sound waves. A patient with unilateral |
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conduction deafness will perceive the sound as com- |
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ing from the affected side (lateralization) because of |
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the lack of masking of environmental noises in that |
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ear (bone conduction). A person with sensorineural |
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deafness, on the other hand, will perceive the sound |
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as coming from the healthy ear because of sound at- |
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tenuation in the affected internal ear. In Rinne’s test, |
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the handle of a tuning fork is placed on one mastoid |
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364 |
process (bony process behind the ear) of the patient |
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(bone conduction). If the tone is no longer heard, the |
tines of the tuning fork are placed in front of the ear (air conduction). Individuals with normal hearing or sensorineural deafness can hear the turning fork in the latter position anew (positive test result), whereas those with conduction deafness cannot (test negative).
The internal ear consists of the equilibrium organ (!p. 342) and the cochlea, a spiraling bony tube that is 3–4 cm in length. Inside the cochlea is an en- dolymph-filled duct called the scala media (cochlear duct); the ductus reuniens connects the base of the cochlear duct to the endolymph-filled part of the equilibrium organ. The scala media is accompanied on either side by two perilymph-filled cavities: the scala vestibuli and scala tympani. These cavities merge at the apex of the cochlea to form the helicotrema. The scala vestibuli arises from the oval window, and the scala tympani terminates on the membrane of the round window (!A2). The composition of perilymph is similar to that of plasma water (!p. 93 C), and the composition of endolymph is similar to that of the cytosol (see below). Perilymph circulates in Corti’s tunnel and Nuel’s spaces (!A4).
Organ of Corti. The (secondary) sensory cells of the hearing organ consist of approximately 10 000–12 000 external hair cells (HCs) and 3500 internal hair cells that sit upon the basilar membrane ( !A4). Their structure is very similar to that of the vestibular organ (!p. 342) with the main difference being that the kinocilia are absent or rudimentary.
There are three rows of slender, cylindrical outer hair cells, each of which contains approximately 100 cilia (actually microvilli) which touch the tectorial membrane. The bases of the hair cells are firmly attached to the basilar membrane by supporting cells, and their cell bodies float in perilymph of Nuel’s spaces (!A4). The outer hair cells are principally innervated by efferent, mostly cholinergic neurons from the spiral ganglion (NM-cholinoceptors; !p. 82). The inner hair cells are pear-shaped and completely surrounded by supporting cells. Their cilia project freely into the endolymph. The inner hair cells are arranged in a single row and synapse with over 90% of the afferent fibers of the spiral ganglion. Efferent axons from the nucleus olivaris superior lateralis synapse with the afferent endings.
Sound conduction in the inner ear. The stapes moves against the membrane of the oval window membrane, causing it to vibrate. These are transmitted via the perilymph to the membrane of the round window (!A2). The walls of the endolymph-filled cochlear duct, i.e. Reissner’s membrane and the basilar mem-
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Despopoulos, Color Atlas of Physiology © 2003 Thieme
All rights reserved. Usage subject to terms and conditions of license.
A. Reception and conduction of sound stimuli |
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Mechanical |
Conduction |
Transduction |
Electrical |
Perception |
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Sound Sensors |
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conduction |
in fluid |
conduction |
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Vestibular |
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organ |
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Air conduction |
Cochlea |
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Sound, |
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Bone conduction |
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of |
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Cochlea |
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Helicotrema |
Conduction |
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2 |
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Unrolled |
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12.28 |
Migrating wave |
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Incus |
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Perilymph |
Plate |
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Malleus |
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Endolymph |
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Stapes |
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Scala |
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Stria |
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vestibuli |
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vascularis |
Spiral |
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Scala |
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media |
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3 |
Scala |
ganglion |
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Scala |
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media |
Scala |
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Auditory |
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tympani |
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vestibuli |
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canal |
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Scala |
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tympani |
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Oval |
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window |
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Tympanic |
Round |
Pharyngeal |
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membrane |
window |
connection |
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External ear |
Middle ear |
Internal ear |
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Tectorial |
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Perilymph |
Scala vestibuli |
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Hair cells |
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membrane |
outer |
inner |
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Reissner’s |
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4 |
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membrane |
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Scala media |
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Afferent and |
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efferent axons |
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Nuel’s |
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Corti’s |
Perilymph |
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Basilar membrane |
365 |
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spaces |
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tunnel |
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Scala tympani |
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Despopoulos, Color Atlas of Physiology © 2003 Thieme
All rights reserved. Usage subject to terms and conditions of license.
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! |
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brane (!D1) give against the pressure wave |
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(migrating wave, !B and C). It can therefore |
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take a “short cut” to reach the round window |
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without crossing the helicotrema. Since the |
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cochlear duct is deformed in waves, Reissner’s |
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membrane and the basilar membrane vibrate |
Senses |
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alternately towards the scala vestibuli and |
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scala tympani (!D1,2). The velocity and |
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wavelength of the migrating wave that started |
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at the oval window decrease continuously |
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and |
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(!B), while their amplitude increases to a |
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System |
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maximum and then quickly subsides (!B, en- |
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velope curve). (The wave velocity is not equal |
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to the velocity of sound, but is much slower.) |
Nervous |
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The site of the maximum excursion of the |
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higher the frequency of the sound, the closer |
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cochlear duct is characteristic of the |
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wavelength of the stimulating sound. The |
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the site is to the stapes (!C). |
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Outer hair cells. Vibration of the cochlear |
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duct causes a discrete shearing (of roughly |
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0.3 nm) of the tectorial membrane against the |
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basilar membrane, causing bending of the cilia |
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of the outer hair cells (!D3). This exerts also a |
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shearing force between the rows of cilia of the |
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individual external hair cell. Probably via the |
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”tip links” (!p. 342), cation channels in the |
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ciliary membranes open (mechanosensitive |
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transduction channels), allowing cations (K+, |
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Na+, Ca2+) to enter and depolarize the outer |
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hair cells. This causes the outer hair cells to |
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shorten in sync with stimulation (!D3). The |
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successive shearing force on the cilia bends |
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them in the opposite direction. This leads to |
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hyperpolarization (opening of K+ channels) |
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and extension of the outer hair cells. |
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The mechanism for this extremely fast electromotil- |
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ity (up to 20 kHz or 2 · 104 times per second) is un- |
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clear, but it seems to be related to the high turgor of |
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outer hair cells (128 mmHg) and the unusual struc- |
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ture of their cell walls. |
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These outer hair cell electromotility con- |
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tributes to the cochlear amplification (ca. 100- |
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fold or 40 dB amplification), which occurs |
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before sound waves reach the actual sound |
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sensors, i.e. inner hair cells. This explains the |
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very low threshold within the very narrow lo- |
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cation (0.5 nm) and thus within a very small |
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frequency range. The electromotility causes |
366 |
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endolymph waves in the subtectorial space |
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which exert shearing forces on the inner hair |
cell cilia at the site of maximum reaction to the sound frequency (!D4), resulting in opening of transduction channels and depolarization of the cells (sensor potential). This leads to transmitter release (glutamate coupling to AMPA receptors; !p. 55 F) by internal hair cells and the subsequent conduction of impulses to the CNS.
Vibrations in the internal ear set off an outward emission of sound. These evoked otoacoustic emissions can be measured by placing a microphone in front of the tympanic membrane, e.g., to test internal ear function in infants and other individuals incapable of reporting their hearing sensations.
Inner ear potentials (!p. 369 C). On the cilia side, the hair cells border with the endolymphfilled space, which has a potential difference (endocochlear potential) of ca. + 80 to + 110 mV relative to perilymph (!p. 369 C). This potential difference is maintained by an active transport mechanism in the stria vascularis. Since the cell potential of outer (inner) hair cells is
– 70 mV (– 40 mV), a potential difference of roughly 150–180 mV (120–150 mV) prevails across the cell membrane occupied by cilia (cell interior negative). Since the K+ conc. in the endolymph and hair cells are roughly equal (!140 mmol/L), the prevailing K+ equilibrium potential is ca. 0 mV (!p. 32). These high potentials provide the driving forces for the influx not only of Ca2+ and Na+, but also of K+, prerequisites for provoking the sensor potential.
Hearing tests are performed using an audiometer. The patient is presented sounds of various frequencies and routes of conduction (bone, air). The sound pressure is initially set at a level under the threshold of hearing and is raised in increments until the patient is able to hear the presented sound (threshold audiogram). If the patient is unable to hear the sounds at normal levels, he or she has an hearing loss, which is quantitated in decibels (dB). In audiometry, all frequencies at the normal threshold of hearing are assigned the value of 0 dB (unlike the diagram on p. 363 B, green curve). Hearing loss can be caused by presbycusis (!p. 362), middle ear infection (impaired air conduction), and damage to the internal ear (impaired air and bone conduction) caused, for example, by prolonged exposure to excessive sound pressure (!90 dB, e.g. disco music, pneumatic drill etc.).
Despopoulos, Color Atlas of Physiology © 2003 Thieme
All rights reserved. Usage subject to terms and conditions of license.
B. Migrating wave in cochlea: maximum amplitude and 3-D topography snapshot
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II |
Distortion of endolymph-filled |
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Sensors |
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cochlear duct |
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+ |
Envelope curve |
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Sound |
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0 |
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– |
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Sound, |
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1 |
2 |
3 |
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Distance from stapes (cm)) |
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of |
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C. Frequency imaging in cochlea |
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Conduction |
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Oval |
700Hz |
Round |
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3000Hz |
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tone |
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tone |
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window |
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window |
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1 |
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12.29 |
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2 |
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Plate |
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3 |
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Cochlea |
Helicotrema |
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cm |
Cochlea |
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(unrolled) |
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(unrolled) |
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D. Stimulation of hair cells by membrane deformation |
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1 |
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2 |
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Cochlear |
Reissner’s membrane |
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duct |
Tectorial membrane |
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Scala vestibuli |
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Scala media |
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Scala tympani |
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3 |
4 |
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Cochlear amplification |
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Sensor potential |
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Tectorial |
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membrane |
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Basilar |
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Outer |
membrane |
Inner |
367 |
hair cells |
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hair cells |
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Despopoulos, Color Atlas of Physiology © 2003 Thieme
All rights reserved. Usage subject to terms and conditions of license.
12 Central Nervous System and Senses
368
Central Processing of Acoustic
Information
Various qualities of sound must be coded for signal transmission in the acoustic pathway. These include the frequency, intensity and direction of sound waves as well as the distance of the sound source from the listener.
Frequency imaging. Tones of various frequencies are “imaged” along the cochlea, conducted in separate fibers of the auditory pathway and centrally identified. Assuming that a tone of 1000 Hz can just be distinguished from one of 1003 Hz (resembling true conditions), the frequency difference of 3 Hz corresponds to a relative frequency differential threshold of 0.003 (!p. 352). This fine differential capacity is mainly due to frequency imaging in the cochlea, amplification by its outer hair cells (!p. 366), and neuronal contrast along the auditory pathway (!p. 313 D). This fine tuning ensures that a certain frequency has a particularly low threshold at its “imaging” site. Adjacent fibers are not recruited until higher sound pressures are encountered.
Intensity. Higher intensity levels result in higher action potential frequencies in afferent nerve fibers and recruitment of neighboring nerve fibers (!A). The relative intensity differential threshold is 0.1 (!p. 352), which is very crude compared to the frequency differential threshold. Hence, differences in loudness of sound are not perceived by the human ear until the intensity level changes by a factor of over 1.1, that is, until the sound pressure changes by a factor of over !1,1 = 1,05.
Direction. Binaural hearing is needed to identify the direction of sound waves and is based on the following two effects. (1) Sound waves that strike the ear obliquely reach the averted ear later than the other, resulting in a lag time. The change in direction that a normal human subject can just barely detect (direction threshold) is roughly 3 degrees. This angle delays the arrival of the sound waves in the averted ear by about 3 · 10-5 s (!B, left). (2) Sound reaching the averted ear is also perceived as being quieter; differences as small as 1 dB can be distinguished. A lower sound pressure results in delayed firing of actions potentials, i.e., in increased latency (!B, right). Thus,
the impulses from the averted ear reach the CNS later (nucleus accessorius, !D5). Effects
(1) and (2) are additive effects (!B). The external ear helps to decide whether the sound is coming from front or back, above or below. Binaural hearing also helps to distinguish a certain voice against high background noise, e.g., at a party. Visibility of the speaker’s mouth also facilitates comprehension.
Distance to the sound source can be determined because high frequencies are attenuated more strongly than low frequencies during sound wave conduction. The longer the sound wave travels, the lower the proportion of high frequencies when it reaches the listener. This helps, for instance, to determine whether a thunderstorm is nearby or far away.
Auditory pathway (!D). The auditory nerve fibers with somata positioned in the spiral ganglion of the cochlea project from the cochlea (!D1) to the anterolateral ( !D2), posteroventral and dorsal cochlear nuclei (!D3). Afferents in these three nuclei exhibit tonotopicity, i.e., they are arranged according to tone frequency at different levels of complexity. In these areas, lateral inhibition (!p. 313 D) enhances contrast, i.e., suppresses noise. Binaural comparison of intensity and transit time of sound waves (direction of sound) takes place at the next-higher station of the auditory pathway, i.e. in the superior olive (!D4) and accessory nucleus (!D5). The next stations are in the nucleus of lateral lemniscus (!D6) and, after most fibers cross over to the opposite side, the inferior quadrigeminal bodies (!D7). They synapse with numerous afferents and serve as a reflex station (e.g., muscles of the middle ear; !p. 366). Here, sensory information from the cochlear nuclei is compared with spatial information from the superior olive. Via connections to the superior quadrigeminal bodies (!D8), they also ensure coordination of the auditory and visual space. By way of the thalamus (medial geniculate body, MGB; !D9), the afferents ultimately reach the primary auditory cortex (!D10) and the surrounding secondary auditory areas (!p. 311 E, areas 41 and 22). Analysis of complex sounds, short-term memory for comparison of tones, and tasks required for “eavesdropping” are some of their functions.
Despopoulos, Color Atlas of Physiology © 2003 Thieme
All rights reserved. Usage subject to terms and conditions of license.
