Cochlea Cross section of the cochlea. Parts of the inner ear, showing the cochlea Gray's subject #232 1050 MeSH Cochlea Dorlands/Elsevier Cochlea
The cochlea is the auditory portion of the inner ear. It is a spiral-shaped cavity in the bony labyrinth, making 2.5 turns around its axis, the modiolus. A core component of the cochlea is the Organ of Corti, the sensory organ of hearing, which is distributed along the partition separating fluid chambers in the coiled tapered tube of the cochlea.
The name is from the Latin for snail shell, which is from the Greek κοχλίας kokhlias ("snail, screw"), from κόχλος kokhlos ("spiral shell") in reference to its coiled shape; the cochlea is coiled in most mammals, monotremes being the exceptions.
The cochlea is a spiralled, hollow, conical chamber of bone, in which waves propagate from the base (near the middle ear and the oval window) to the apex (the top or center of the spiral). Its structures include:
- Three scalae or chambers:
- the scala vestibuli (containing perilymph), which lies superior to the cochlear duct and abuts the oval window
- the scala tympani (containing perilymph), which lies inferior to the scala media and terminates at the round window
- the scala media (containing endolymph), or cochlear duct, a region of high potassium ion concentration that the cilia of the hair cells project into
- The helicotrema, the location where the scala tympani and the scala vestibuli merge, at the apex of the cochlea
- Reissner's membrane, which separates the scala vestibuli from the scala media
- The basilar membrane, a main structural element that separates the scala media from the scala tympani and determines the mechanical wave propagation properties of the cochlear partition
- The Organ of Corti, the sensory epithelium, a cellular layer on the basilar membrane, in which sensory hair cells are powered by the potential difference between the perilymph and the endolymph
- hair cells, sensory cells in the Organ of Corti, topped with hair-like structures called stereocilia
The walls of the hollow cochlea are made of bone, with a thin, delicate lining of epithelial tissue. This coiled tube is divided through most of its length by an inner membranous partition. Two fluid-filled outer spaces (scalae) are formed by this dividing membrane. The fluid in both of these ouiding membrane. This continuation at the helicotrema allows fluid being pushed into the scala vestibuli by the oval window to move back out via movement in scala tympani and deflection of the round window; since the fluid is nearly incompressible and the bony walls are rigid, it is essential for the conserved fluid volume to exit somewhere.
The lengthwise partition that divides most of the cochlea is itself a fluid-filled tube, the third scala. This central column is called the scala media, or cochlear duct. Its fluid, endolymph, also contains electrolytes and proteins, but is chemically quite different from perilymph. Whereas the perilymph is rich in sodium ions, the endolymph is rich in potassium ions, which produces an ionic, electrical potential.
The hair cells are arranged in four rows in the organ of Corti along the entire length of the cochlear coil. Three rows consist of outer hair cells (OHCs) and one row consists of inner hair cells (IHCs). The inner hair cells provide the main neural output of the cochlea. The outer hair cells, instead, mainly receive neural input from the brain, which influences their motility as part of the cochlea's mechanical pre-amplifier. The input to the OHC is from the olivary body via the medial olivocochlear bundle.
The cochlear duct is almost as complex on its own as the ear itself. It is bounded on its three sides by the basilar membrane, the stria vascularis, and Reissner's membrane. Stria vascularis is a rich bed of capillaries and secretory cells; reissner's membrane is a thin membrane that just separates endolymph from perilymph; and the basilar membrane is a mechanically somewhat stiff membrane, supporting the receptor organ for hearing, the organ of Corti, and determines the mechanical wave propagration properties of the cochlear system.
The cochlea is filled with a watery liquid, the perilymph, which moves in response to the vibrations coming from the middle ear via the oval window. As the fluid moves, the cochlear partition (basilar membrane and organ of Corti) moves; thousands of hair cells sense the motion via their cilia, and convert that motion to electrical signals that are communicated via neurotransmitters to many thousands of nerve cells. These primary auditory neurons transform the signals into electrochemical impulses known as action potentials, which travel along the auditory nerve to structures in the brainstem for further processing.
The stapes (stirrup) ossicle bone of the middle ear transmits vibrations to the fenestra ovalis (oval window) on the outside of the cochlea, which vibrates the perilymph in the scala vestibuli (upper chamber of the cochlea). The ossicles are essential for efficient coupling of sound waves into the cochlea, since the cochlea environment is a fluid–membrane system, and it takes more pressure to move sound through fluid–membrane waves than it does through air; a pressure increase is achieved by the area ratio of the tympanic membrane to the oval window, resulting in a pressure gain of about 20× from the original sound wave pressure in air. This gain is a form of impedance matching – to match the soundwave travelling through air to that travelling in the fluid–membrane system.
At the base of the cochlea, each scala ends in a membranous portal that faces the middle ear cavity: The scala vestibuli ends at the oval window, where the footplate of the stapes sits. The footplate vibrates when the pressure is transmitted via the ossicular chain. The wave in the perilymph moves away from the footplate and towards the helicotrema. Since those fluid waves move the cochlear partition that separates the scalae up and down, the waves have a corresponding symmetric part in perilymph of the scala tympani, which ends at the round window, bulging out when the oval window bulges in.
The perilymph in scala vestibuli and the endolymph in scala media act mechanically as a single duct, being kept apart only by the very thin Reissner's membrane. The vibrations of the endolymph in the scala media displace the basilar membrane in a pattern that peaks a distance from the oval window depending upon the soundwave frequency. The organ of Corti vibrates due to outer hair cells further amplifying these vibrations. Inner hair cells are then displaced by the vibrations in the fluid, and depolarise by an influx of K+ via their tip-link-connected channels, and send their signals via neurotransmitter to the primary auditory neurons of the spiral ganglion.
The hair cells in the organ of Corti are tuned to certain sound frequencies by way of their location in the cochlea, due to the degree of stiffness in the basilar membrane. This stiffness is due to, among other things, the thickness and width of the basilar membrane, which along the length of the cochlea is stiffest nearest its beginning at the oval window, where the stapes introduces the vibrations coming from the eardrum. Since its stiffness is high there, it allows only high-frequency vibrations to move the basilar membrane, and thus the hair cells. The farther a wave travels towards the cochlea's apex (the helicotrema), the less stiff the basilar membrane is; thus lower frequencies travel down the tube, and the less-stiff membrane is moved most easily by them where the reduced stiffness allows: that is, as the basilar membrane gets less and less stiff, waves slow down and it responds better to lower frequencies. In addition, in mammals, the cochlea is coiled, which has been shown to enhance low-frequency vibrations as they travel through the fluid-filled coil. This spatial arrangement of sound reception is referred to as tonotopy.
For very low frequencies (below 20 Hz), the waves propagate along the complete route of the cochlea – differentially up scala vestibuli and scala tympani all the way to the helicotrema. Frequencies this low still activate the organ of Corti to some extent, but are too low to elicit the perception of a pitch. Higher frequencies do not propagate to the helicotrema, due to the stiffness-mediated tonotopy.
A very strong movement of the basilar membrane due to very loud noise may cause hair cells to die. This is a common cause of partial hearing loss and is the reason why users of firearms or heavy machinery often wear earmuffs or earplugs.
Amplification by the hair cells
Not only does the cochlea "receive" sound, it generates and amplifies sound when it is healthy. Where the organism needs a mechanism to hear very faint sounds, the cochlea amplifies by the reverse transducer of the OHCs, converting electrical signals back to mechanical in a possitive-feedback configuration. The OHCs have a protein motor called prestin on their outer membranes; it generates additional movement that couples back to the fluid–membrane wave. This "active amplifier" is essential in the ear's ability to amplify weak sounds.
The active amplifier also leads to the phenomenon of soundwave vibrations being emitted from the cochlea back into the ear canal (otoacoustic emissions).
Otoacoustic emissions are due to a wave exiting the cochlea via the oval window, and propagating back through the middle ear to the eardrum, and out the ear canal, where it can be picked up by a microphone. Otoacoustic emissions are important in some types of tests for hearing impairment, since they are present when the cochlea is working well, and less so when it is suffering from loss of OHC activity.
The coiled form of cochlea is unique to mammals. In birds and in other non-mammalian vertebrates, the compartment containing the sensory cells for hearing is occasionally also called “cochlea,” despite not being coiled up. Instead, it forms a blind-ended tube, also called the cochlear duct. This difference apparently evolved in parallel with the differences in frequency range of hearing and in frequency resolution between mammals and non-mammalian vertebrates. Most bird species do not hear above 4–5 kHz, the currently known maximum being ~ 11 kHz in the barn owl. Some marine mammals hear up to 200 kHz. The superior frequency resolution in mammals is due to their unique mechanism of pre-amplification of sound by active cell-body vibrations of outer hair cells. A long coiled compartment, rather than a short and straight one, provides more space for mapping pitches, so is therefore better adapted to the highly derived functions in mammalian hearing.
As the study of the cochlea should fundamentally be focused upon the level of hair cells, it is important to note the anatomical and physiological differences between the hair cells of various species. In birds, for instance, instead of outer and inner hair cells, there are tall and short hair cells. There are several similarities of note in regard to this comparative data. For one, the tall hair cell is very similar in function to that of the inner hair cell, and the short hair cell is very similar in function to that of the outer hair cell. One unavoidable difference, however, is that while all hair cells are attached to a tectorial membrane in birds, only the outer hair cells are attached to the tectorial membrane in mammals.
In 2009, engineers at the Massachusetts Institute of Technology created an electronic chip that can quickly analyze a very large range of radio frequencies while using only a fraction of the power needed for existing technologies; its design specifically mimics a cochlea.
- Cochlear implant
- Cochlear nerve
- Cochlear nuclei
- Noise health effects
- Cochlear virus
- Cochlear implosions
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- ^ Vater M, Meng J, Fox RC. Hearing organ evolution and specialization: Early and later mammals. In: GA Manley, AN Popper, RR Fay (Eds). Evolution of the Vertebrate Auditory System, Springer-Verlag, New York 2004, pp 256–288.
- ^ Anne Trafton (June 3, 2009). "Drawing inspiration from nature to build a better radio: New radio chip mimics human ear, could enable universal radio". MIT newsoffice. http://web.mit.edu/newsoffice/2009/bio-electronics-0603.html.
- ^ Soumyajit Mandal, Serhii M. Zhak, and Rahul Sarpeshkar (June 2009). "A Bio-Inspired Active Radio-Frequency Silicon Cochlea". IEEE Journal of Solid-State Circuits 44 (6): 1814–1828. doi:10.1109/JSSC.2009.2020465.
- Physiology of the Ear By Anthony F. Jahn, Joseph Santos-Sacchi
- Audiology By Ross J. Roeser, Michael Valente, Holly Hosford-Dunn
- Audition By Michel Imbert, R. H. Kay
- The Cochlea By Peter Dallos, Arthur N. Popper, Richard R. Fay
- MeSH Cochlea
- "Promenade 'Round the Cochlea" by R. Pujol, S. Blatrix, T. Pujol et al. at University of Montpellier
- "The Cochlea Homepage", F. Mammano and R. Nobili of the Venetian Institute of Molecular Medicine
- MYSTERIES OF THE COCHLEA Dr. Janez Faganel Memorial Lecture at University Medical Centre Ljubljana
Sensory system: Auditory and Vestibular systems (TA A15.3, TH 3.11.09, GA 10.1029) Outer ear Middle ear
Tegmental wall/roof: Epitympanic recessJugular wall/floorStapedius · Tensor tympani
bony labyrinth)General cochleaPerilymphatic spaceCells
- Three scalae or chambers:
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