Figure - available from: Biomechanics and Modeling in Mechanobiology
This content is subject to copyright. Terms and conditions apply.
The human cochlea and cochlear mechanics under air and bone conduction. a The human cochlea with air and bone conduction pathways. The cochlea is a spiral, fluid-filled organ surrounded by bony structures. It connects the stapes of the middle ear at the oval window (OW). Under air conduction, the sound energy enters the cochlea through the OW, while under bone conduction, the sound energy enters the cochlea mostly through the bony walls. b Vibration patterns of the cochlear walls under bone conduction. At low frequency, the rigid body motion (RBM) dominates; as the stimulating frequency increases, the compressional motion (CPM) becomes significant. The RBM does not change the cochlear volume, while the CPM alters the cochlear inner space. c A sketch of the cochlea and the traveling wave (TW). In the mechanical perspective, the cochlea is simplified as two fluid chambers (scala vestibula, SV and scala tympani, ST) separated by the basilar membrane (BM). SV and ST connect at the apical end of the cochlea, named helicotrema. At the base of the cochlea, the oval window (OW) and stapes abuts SV, and the round window (RW) abuts ST. Under both air and bone conduction stimulations, the traveling wave (TW) emerges at the BM and travels from the basal end toward the apical end. The TW amplitude peaks under pure tone stimulations, and the peak location depends on the sound frequency

The human cochlea and cochlear mechanics under air and bone conduction. a The human cochlea with air and bone conduction pathways. The cochlea is a spiral, fluid-filled organ surrounded by bony structures. It connects the stapes of the middle ear at the oval window (OW). Under air conduction, the sound energy enters the cochlea through the OW, while under bone conduction, the sound energy enters the cochlea mostly through the bony walls. b Vibration patterns of the cochlear walls under bone conduction. At low frequency, the rigid body motion (RBM) dominates; as the stimulating frequency increases, the compressional motion (CPM) becomes significant. The RBM does not change the cochlear volume, while the CPM alters the cochlear inner space. c A sketch of the cochlea and the traveling wave (TW). In the mechanical perspective, the cochlea is simplified as two fluid chambers (scala vestibula, SV and scala tympani, ST) separated by the basilar membrane (BM). SV and ST connect at the apical end of the cochlea, named helicotrema. At the base of the cochlea, the oval window (OW) and stapes abuts SV, and the round window (RW) abuts ST. Under both air and bone conduction stimulations, the traveling wave (TW) emerges at the BM and travels from the basal end toward the apical end. The TW amplitude peaks under pure tone stimulations, and the peak location depends on the sound frequency

Source publication
Article
Full-text available
Besides the normal hearing pathway known as air conduction (AC), sound can also transmit to the cochlea through the skull, known as bone conduction (BC). During BC stimulation, the cochlear walls demonstrate rigid body motion (RBM) and compressional motion (CPM), both inducing the basilar membrane traveling wave (TW). Despite numerous measuring and...

Citations

... In the box model, the cochlea is straightened and includes the upper and lower cavities (scala vestibuli and scala tympani) separated by the BM. The arrangement of the spiral model is similar to the box model, but the geometry incorporates cochlea coiling (45,46). ...
... Some studies of the inner ear model have applied mechanical stimulation on the OW to study the cochlear response (46,59). In some middle ear models, the cochlea was assumed as a mass, and stimulation was applied to the eardrum to study the middle ear transfer function (40,(60)(61)(62). ...
Article
Full-text available
Background and objective: An auditory prosthesis refers to a device designed to restore hearing. Some parameters of the auditory prosthesis, such as mass, implanted position, and degree, need to be repeatedly designed and optimized based on the realistic geometry of the ear. Numerous auditory prostheses designs were based on animal or specimen experiments involving many complex instruments, and the experimental specimens had low repeatability. The finite element method (FEM) can overcome these disadvantages and be carried out on the computer with substantial flexibility in modifying the prosthetic parameters to optimize them. This narrative review aims to analyze the recent advances in the design and optimization of auditory prostheses using the FEM and provides suggestions for future development. Methods: The literature on the design of auditory prostheses using the FEM has been extensively studied using the PubMed and Web of Science databases, including different ear models and relevant parameters of different auditory prostheses that need to be designed and optimized. Key content and findings: The process of designing and optimizing a prosthesis using the FEM includes building an ear model and a prosthesis model to simulate the implantation process. The related parameters of the prosthesis can be designed and modified conveniently. The post-implantation response could be used as an indicator to evaluate the prosthesis's performance. Conclusions: The review concluded that the FEM had been widely studied in designing and optimizing middle ear implants and cochlear implants and obtained good results. FEM can be utilized to explore more effective directions for auditory prosthesis design and optimization in the future.