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22
S. Dayisoylu et al.
2.4 Embryology oftheCochlear Nerve andCentral
Auditory Pathways
Embryologically, the vestibulocochlear ganglion (acoustic vestibular ganglion) and the seventh nerve ganglion (facial ganglion) rst unite. The three parts separate one after the other throughout time. Unlike other sensory ganglia in the brain, which derive neuroblasts from both neural crest placodes and ganglionic cells, the otocyst epithelium is the sole source of neuroblasts in the vestibular and cochlear (acoustic) ganglia. All cranial ganglia have the characteristic that their supporting Schwann and satellite cells are completely neural crest-originated, most likely deriving from the facial nerve ganglion [1722].

References

1. Bhatt RA.Ear anatomy. In: Gest TR, editor. Medscape; 2016. Updated: Jun 27, 2016. https://
emedicine.medscape.com/article/1948907- overview#a4. Accessed online on July 23, 2023.
2. Honrado CP, Bradley DT, Larrabee WF. Embryology of the external ear. In: Azizzadeh B, Murphy M, Johnson C, editors. Master techniques in facial rejuvenation. Saunders; 2007. p.17–32.
3. Ear PF.Sobotta Atlas of human anatomy, vol. 3. 23rd. ed. Elsevier GmbH; 2010. p.133–60.
4. Bruss DM, Shohet JA.Neuroanatomy, ear. [Updated 2023 Apr 3]. In: StatPearls. Treasure Island (FL): StatPearls Publishing; 2023. Available from: https://www.ncbi.nlm.nih.gov/
books/NBK551658/ (Accessed online on July 23, 2023).
5. Whiteld TT.Development of the inner ear. Curr Opin Genet Dev. 2015;32:112–8.
6. Fuchs JC, Tucker AS. Development and integration of the ear. Curr Top Dev Biol. 2015;115:213–32.
7. Anniko M, Wikström SO.Pattern formation of the otic placode and morphogenesis of the otocyst. Am J Otolaryngol. 1984;5(6):373–81.
8. Patel PK.Head and neck embryology. In: Narayan D, editor. Medscape; 2021. Updated: Dec 21, 2021. https://emedicine.medscape.com/article/1289057- overview#a1 (Accessed online on July 23, 2023).
9. Moore KL, Persaud TVN, Torchia MG.The developing human: clinically oriented embryol­ogy. 10th ed. Philadelphia, PA: Elsevier; 2016.
10. Schoenwolf GC, Bleyl SB, Brauer PR, Francis-West PH.Larsen’s human embryology. 5th ed. Philadelphia, PA: Churchill Livingstone; 2015.
11. Langman J.Medical embryology. Baltimore, MD: Williams and Wilkins; 1981.
12. Roth DM, Bayona F, Baddam P, Graf D.Craniofacial development: neural crest in molecular embryology. Head Neck Pathol. 2021;15(1):1–15.
13. Carstens MH. Neural tube programming and craniofacial cleft formation. I. The neuro­meric organization of the head and neck. Eur J Paediatr Neurol. 2004;8(4):181–210. discus­sion 179–80
14. DeMyer WE, Zeman W, Palmer CG.The face predicts the brain: diagnostic signicance of median facial anomalies for holoprosencephaly (arrhinencephaly). Pediatrics. 1964;34:256–63.
15. Carstens MH.Development of the facial midline. J Craniofac Surg. 2002;13(1):129–87. dis­cussion 188–90
16. Hashimoto C, Kitamura K, Yamamoto M, etal. Auricular cartilage conguration: a histologi­cal study using late-stage human fetuses and adult cadavers. Anat Rec (Hoboken). 2021;
17. Tewk TL.Auditory system anatomy. In: Gest TR, editor. Medscape; 2017. Updated: Dec 08,
2017. https://emedicine.medscape.com/article/1948643- overview#a2 (Accessed online at July 23, 2023).
2 Outer–Middle–Inner Ear Embryology
18. Kandel ER, Schwartz JH, Jessell TM. Principles of neuroscience. 4th ed. New York, NY: McGraw-Hill; 2000. p.591–624.
19. Johnston MC. Developmental biology of the ear. In: Tewk TL, Der Kaloustian VM, edi­tors. Congenital anomalies of the ear, nose, and throat. NewYork, NY: Oxford University Press; 1997.
20. Josey AF, Glasscock ME 3rd, Musiek FE.Correlation of ABR and medical imaging in patients with cerebellopontine angle tumors. Am J Otol. 1988;9:12–6.
21. Ferguson MA, Smith PA, Lutman ME, Mason SM, Coles RR, Gibbin KP. Efciency of tests used to screen for cerebello-pontine angle tumours: a prospective study. Br J Audiol. 1996;30(3):159–76.
22. Lonsbury-Martin BL, Martin GK, Coats AC.Chapter 47: The physiology of the auditory and vestibular systems. In: Ballenger JJ, editor. Diseases of the nose, throat, ear, head and neck. 13th ed. Philadelphia, PA: Lea and Febiger; 1985. p.952–4.
23
Physiology ofthePeripheral andCentral Hearing System
MustafaBaran, ErdoğanBulut, ŞerefErdoğan, andAtrurLorens

3.1 Introduction

This chapter provides a comprehensive overview of the auditory system, with spe­cial emphasis on the peripheral and central parts of hearing. The journey of sound perception begins with the synchronized movement of anatomical structures. This orchestrated sequence is critical to the transformation of sound waves into percep­tible sounds.
The conduction phase of hearing primarily involves the outer and middle ear. The outer ear, consisting of the auricle (pinna) and the external ear canal, acts as the initial receiver of sound waves. The pinna, with its unique shape and structure, helps capture the sound waves and directs them through the ear canal to the eardrum. This stage involves not only the transmission of sound but also the initial amplication and localization of these sound waves, preparing them for further processing. The middle ear, which contains the ossicular chain (malleus, incus, and stapes), serves
3
M. Baran Medical Faculty, Department of Physiology, Istanbul Medeniyet University, Istanbul, Turkey e-mail: mustafa.baran@batman.edu.tr
E. Bulut (*) Faculty of Health Sciences, Department of Audiology, Trakya University, Edirne, Turkey
Faculty of Medicine, Department of Physiology, Trakya University, Edirne, Turkey Trakya University, Mirko TOS Ear & Hearing Research Center, Edirne, Turkey
e-mail: erdoganbulut@trakya.edu.tr Ş. Erdoğan
Medical Faculty, Department of Physiology, Cukurova University, Adana, Turkey e-mail: serdogan@cu.edu.tr
A. Lorens Implants and Auditory Perception Department, World Hearing Center, Institute of Physiology and Pathology of Hearing, Nadarzyn, Poland e-mail: a.lorens@ifps.org.pl
© The Author(s), under exclusive license to Springer Nature Switzerland AG 2024 M. T. Kalcioglu et al. (eds.), Otology Updates, Comprehensive ENT,
https://doi.org/10.1007/978-3-031-76173-7_3
25
26
as a mechanical amplier, transmitting vibrations from the eardrum to the oval win­dow of the cochlea. Efcient transmission of these vibrations is essential for the subsequent conversion stage, and any disruption in this stage can result in conduc­tive hearing loss.
The conversion stage takes place in the inner ear, specically in the cochlea, a uid-lled spiral organ that is the cornerstone of auditory transduction. In the cochlea, the mechanical energy of sound vibrations is converted into electrical sig­nals by delicate hair cells. These signals are then transmitted via the eighth nerve to the auditory cortex, where sound is perceived and interpreted. This conversion from mechanical to electrical energy is a critical step in the auditory process, and disrup­tions in this stage can result in sensorineural hearing loss. Understanding these stages and their components is crucial for diagnosing different types of hearing loss. For example, problems in the outer or middle ear that affect sound conduction can lead to conductive hearing loss, while problems in the inner ear, particularly with hair cells or the auditory nerve, can cause sensorineural hearing loss. In addition, this detailed understanding of the function of the auditory system facilitates the development of targeted interventions, ranging from hearing aids that amplify sound to cochlear implants that stimulate the auditory nerve directly, bypassing damaged parts of the ear.
M. Baran et al.
3.2 The Peripheral Auditory System: APerspective
The perception of sound stimuli occurs through the synchronized movement of ana­tomical formations, beginning with the outer ear and extending into the middle and inner ear. [1]. Within the auditory system, the outer and middle ear participate in the conduction phase, while the inner ear participates in the conversion phase. These stages are critical for classifying hearing loss.

3.3 The Outer Ear

3.3.1 Anatomy
The outer ear consists of the auricle (pinna), which contains a resonance cavity called the concha, and the external ear canal. The external ear canal begins at the pinna and runs to the tympanic membrane (TM) and is in the form of a tube closed at one end (Fig.3.1) [2]. The lateral (one-third) part of the external ear canal con­sists of brocartilage tissue, and the medial (two-third) part consists of the temporal bone. The isthmus region, where the cartilage and bone parts meet, is the narrowest part of the external ear canal and is the area where external objects are most likely to get stuck. The cerumen of the external ear canal, which is the skin portion of the sweat and sebaceous glands that form earwax, is covered with hair. As the hair grows outward, it joins the cerumen to form a disinfectant and defensive barrier within the external ear canal [3, 4]. The dimensions and shape of the external ear
3 Physiology ofthePeripheral andCentral Hearing System
Fig. 3.1 The outer ear
27
canal determine the sound pressure in front of the TM and the transmission function of sound. Knowledge of its anatomy is essential to compare, optimize, and advance acoustic measurement methods [3]. It also allows for good hearing aid tting [5].
3.3.2 Resonance andAmplification
The external ear canal runs from the top and back to the bottom and front. The shape of the canal corresponds to an S-shaped conduction path in the coronal plane [3]. Therefore, during otoscopic examination, the external ear canal is straightened by pulling the auricle backward and upward and an image of the TM is obtained [6]. The geometry of the external ear canal is determined by the parameters of length, radius, and cavity shape, which vary from person to person. From birth to 7years of age, a really big change in canal volume and length is observed in the external ear canal, and, after that, the canal characteristics are comparable to those of adults [3]. Information on the geometry of the external ear canal in adults is based on measure­ments made by Stinson and Lawton on the right external ear canal of 15 human cadavers, which will serve as a source for future studies [7]. Although there are biological differences between individuals, the outer ear canal is approximately 25–32mm in length. The cross-sectional area ranges from 90.13 to 96.16mm2 at the entrance of the canal and from 65.45 to 75.53mm2 at the TM [8]. The average ear canal volume is 0.62ml, and, in children under 7years of age, it is 0.37ml [2]. The effect of the outer ear on the incoming sound can be analyzed in two ways: First, it is the resonance effect of the outer ear on the sound pressure at the TM and the resulting amplication. In addition, it affects directional hearing by providing
28
M. Baran et al.
information about the localization of the sound source [9]. Under the resonance effect, the auricle and concha collect sounds over a wide area and transmit them to the narrowed external ear canal. In humans, these sounds produce a peak at around
2.5kHz with an amplication of about 15–20dB, causing an increase in pressure on the TM.However, the maximum increase is approximately 17–22dB at 3 kHz. Subsequently, this increase creates a maximum resonance within the TM at 3kHz and its multiples [10]. In infants, the resonance frequency is approximately 6–7kHz [9, 11]. This is the result of the combined resonance effects of the concha and the pinna. The resonant frequency of the concha alone is about 5.5kHz, showing that the concha is dependent on high frequencies for sound pressure changes. For sound transmission in air, the wavelength is 1.56mm at 20kHz and 15.6 mm at 20 Hz [11]. This is usually an indication of how important the pinna is to us in the audible frequency range. The resonant frequency of the external ear canal is between 2.5 and 4kHz. Depending on pressure changes, the resonance of the outer ear changes between 1.5kHz and 7kHz [1, 11].
3.3.3 Localization
A sound source is located in three spatial dimensions. First, it can be located within the horizontal plane (azimuth-horizon angle), that is right and left, and, second, it can be located above or below within the vertical plane. Third, there is distance, i.e., near and far sound sources [11]. For this reason, time (interaural time difference) and intensity (interaural level difference) differences within the sound waves arriv­ing at the two ears provide critical cues within the localization of the sound source [1]. In the horizontal plane, time and phase differences in the time it takes for the sound to reach the ear closest to the source versus the ear farthest away.
Considering that sound has no spatial dimension and its speed in air is indepen­dent of frequency (sound speed at 20 °C; 1atm pressure is 343m/s), when a tonal stimulus is presented to one ear (0.5kHz and 1kHz), the sound is delayed by 0.5ms (interaural time difference) to the other ear and arrives with a phase difference [9,
11]. This allows low-frequency sounds to be localized to the nearest ear. In humans,
the auricle provides a large directional selectivity for high frequencies, and at 6kHz and above, it provides a gain of 10–15dB at an angle of 70°, depending on the fre­quency, with the head in a straight position [9]. Although it is assumed that the sound stimulus is collected by the auricle and directed to the TM, the head and body of the individual also play a role in this mechanism. The head, the chest, the auricle, where the incoming stimulus strikes; before the sound reaches the TM, it amplies the sounds adapted to the resonance frequency or creates a barrier and reduces their intensity. The angle of incidence and the frequency of the sound stimulus are factors in this mechanism [1]. It is known that the azimuth effect produces a gain of about 6dB for sounds coming from 45° and 90° angles. When the intensity between the ears is known, the shadow effects of the head on the sound are critical. On the side where the sound is coming from, the sound waves that hit the head are reected and then refracted. This increases the sound pressure in the ear on that side (bafe effect)
3 Physiology ofthePeripheral andCentral Hearing System
and decreases the sound pressure by blocking the head sound waves in the ear on the opposite side of the sound direction (acoustic shadow). The shadow effect depends on the frequency of the sound. For high-frequency sounds, the wavelength is short and the shadow effect of the head is large. The intensity difference between the ears can be a factor in determining the localization of the sound source at high frequen­cies [1, 9, 11].
29

3.4 The Middle Ear

3.4.1 Structural Elements andTheir Functions
The middle ear (Fig.3.2a) is located in the cavity within the temporal bone (tym­panic cavity—tympanum) and may be a site where there is a continuous ow of air connected to the air-lled mastoid cells via the Eustachian tube and to the external environment via the aditus ad antrum. This is important for the conductive function of the middle ear [9, 11]. It is structurally separated from the outer ear by the TM.The TM is connected to the oval window of the inner ear by the ossicular chain. There are two muscles and ligaments on the ossicular chain that are critical to its physiological function [1113].
3.4.2 The Tympanic Membrane andtheOssicular Chain
The TM is located in the last part of the external ear canal and, due to the different lengths of the canal walls, forms an angle of 140° with the upper and posterior canal walls and an angle of 30° with the lower and anterior canal walls. This tilt or orien­tation gives the TM a usable area of approximately 85mm2. The periphery of the TM (Fig.3.2b), approximately more than 270°, is tightly connected to the tympanic cavity/annular sulcus by a brocartilaginous ring called the tympanic annulus or the annular ligament [9, 14]. The lower part of the TM that attaches to the annular sul­cus is called the pars tensa and constitutes three-fourth of the membrane. The pars tensa shows a multilaminar layering with circular bers extending throughout the tympanic layer and radial bers extending to a lesser extent and appearing as a species-specic variety. The pars accida is located above the TM and is anatomi­cally and functionally distinct from the pars tensa. It attaches to the Rivinus notch within the annular sulcus at the superior part of the tympanic ring. It constitutes one-fourth of the membrane, and, although its dimensions are different in mam­mals, it is thicker than the pars tensa and does not have brous organization. In rapid vibration of the tympanic membrane, mass distribution, such as thickness, may be a critical property for vibrational behavior [8, 12]. In their study of three fresh human cadavers, Kuypers etal. found that the mean thickness values of the TM showed incredible interindividual variation (40, 50, and 120μm). In any case, the authors expressed that variations in thickness are common to all individuals [15]. Appropriately, they expressed that the inferior-posterior quadrant of the TM is
30
M. Baran et al.
a
b
c
Fig. 3.2 (a) Middle ear (tympanic cavity of guinea pig) magnication: 15×1.5×11.1. (b) Guinea pig tympanic membrane with an annular structure; magnication: 15×1.5×11.4. (c) Morphology of the tympanic membrane
largely thinner and becomes progressively thicker toward the superior part, with the anterior part being thicker than the posterior part. In histological sections of the TM, it has been suggested that the membrane may be a multilayered brous structure containing different layers of varying thickness and density [16]. The TM is three­layered. Its innermost layer includes the inner mucosal epithelial layer, which con­tains an extremely thin layer of cells on its medial side, the outer epidermal layer, which is the continuation of the external ear canal epidermis on the lateral side, and the brous layer or lamina propria in the middle. The lamina propria of the pars tensa contains two subepidermal layers and two collagen layers organized into radial and circular bers; while radial bers extend from the TM toward the
3 Physiology ofthePeripheral andCentral Hearing System
31
periphery (converging at the manubrium), circular bers thicken and lengthen toward the periphery [8]. In a study by O’Connor etal., as shown in Fig.3.2c, they expressed that radial collagen bers play an important role in high-frequency sounds, especially 4kHz and above, and circular bers play a critical role in low­frequency responses [17]. The TM is attached to the arm of the malleus (manu­brium) and the umbo but is more loosely attached to the manubrium. The ossicular chain extends medial to the TM [18].
The primary ossicle consists of the malleus (anvil), head, neck, manubrium, and umbo. The head extends toward the epitympanum and articulates with the body of the incus. The anterior projection of the neck is the point of attachment of the tensor tympani muscle. The incus is the median bone and has short and long arms and a lenticular process. The lenticular process may be a attened bone that connects to the head of the stapes [12]. The stapes is the smallest bone in the body. It consists of a head, two legs (anterior and posterior crus), and a base called the footplate, which is connected to the oval window by the annular ligament. Thus, the ossicular chain connects the outer ear to the inner ear directly through the TM [11].
3.4.3 Middle Ear Muscles
The middle ear muscles control the transmission of sound through the middle ear. The ossicles are connected to two small, striated muscles. The rst is the tensor tympani, which is 25-mm-long in adults and runs parallel to the Eustachian tube, most of which lies within the bony canal. Its tendon is attached to the malleus, and its innervation is the trigeminal nerve known as the fth cranial nerve. It reduces the tension of the TM to high intensity sounds, making the inner ear less sensitive to sound. The second is the stapes muscle and is located in a bone canal, and its tendon is attached to the stapes head. Its length is 6mm. It is innervated by the facial nerve, known as the seventh cranial nerve. Its contraction moves the base of the stapes away from the oval window, preventing loud sounds from reaching the inner ear [9,
11, 12]. Contraction of the middle ear muscles increases the stiffness of the ossicu-
lar chain. Sound transmission through the middle ear below 1 and 2kHz is provided by the stiffness of the ossicular chain. Stiffness also results from the compression and expansion of air in the middle ear as well as the elasticity of the TM and the ligaments of the ossicular chain. Stiffness decreases with transmission of low­frequency sounds. In other words, as the stiffness of the ossicular chain increases, the response to low-frequency sounds decreases. Above 1 and 2kHz, the middle ear muscles are less effective in transmitting sound and transmission does not occur with ossicular chain stiffness [9]. Middle ear muscle contraction may occur as a reex (stapes or tympanic reex) in response to high-intensity sounds (75dB and above the hearing threshold), or this response may also occur during speech, tactile stimulation of the head, swallowing, and general body movements. Many functions of the middle ear muscles have been proposed [1, 9, 11].
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M. Baran et al.
– The reex contraction of the middle ear muscles at high-intensity sounds pro-
tects the inner ear from acoustic trauma caused by noise.
– For high-intensity, low-frequency stimuli, the middle ear muscles keep the high-
intensity sound constant in the lower part of the intensity range, providing near-
perfect automatic amplication of low-frequency responses as the sound enters
the cochlea. In other words, to protect the inner ear from high-intensity stimuli,
the contraction of the stapes muscle provides a 10–20-dB gain reduction for
80–90-dB stimuli. The maximum contraction of the stapes muscle occurs on
average 63ms after the stimulus reaches the ear. It is suggested that the tensor
tympani muscle protects the inner ear by limiting the movement of the ossicular
chain with its contractile motion against loud sounds.
– The middle ear muscles also affect the frequency response of the middle ear.
Muscle contraction varies with frequency.
– High-intensity, low-frequency stimulation can mask the high-frequency stimula-
tion response over a wide frequency range by contracting the middle ear muscles.
3.4.4 The Eustachian Tube
The Eustachian tube was rst described in detail by Bartolomeo Eustachius in
1552. However, the real discoverer was a scientist named Alcmaeon in 1500BC.He studied the Eustachian tube, middle ear, and pharynx and stated that the tensor tym­pani and the ossicular chain play a critical role in the sound transmission mecha­nism [18]. The middle ear consists of a cavity within the bones of the head. It is closed medially by the TM and laterally by the oval window. In order for the TM to achieve some exibility during sound transmission, pressure must be generated by lling and emptying the middle ear with air. This function is performed by the Eustachian tube [1]. The Eustachian tube is a canal that connects the middle ear to the nasopharynx (Fig.3.3). It is 35–40-mm-long. Two-thirds of its anteromedial part is cartilage (24mm), and one-third of its posterolateral part is bone (11mm). The part called the isthmus is the narrowest part of the Eustachian tube. Although it is horizontal at birth, it has an angle of 450in adults. In infants, it is about 18mm and more horizontal. The tensor and levator veli palatini are the muscles of the Eustachian tube. The tensor veli palatini is the muscle that plays an active role in opening the tube. This muscle is made up of white bers that are strong and fast twitching. These bers make up 60% of the muscle, while the remaining 40% is made up of red, slow, long-twitch bers. The levator veli palatini muscle does not have a direct effect on the opening and closing of the Eustachian tube because it is located at a considerable distance from the tube. In this muscle, white muscle bers and slow and long twitch red bers are found equally. In some people, the Eustachian tube is constantly closed, which is pathological. In this case, movements of the TM can be observed with an otoscope with every breath [1, 12, 19]. When the Eustachian tube is open, the air in the middle ear and the air in front of the TM are equalized, making the TM receptive to incoming stimuli. At high altitudes, the external envi­ronmental pressure, and therefore the external ear pressure, decreases. In this case,