<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.xsl"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-09-21T02:22:33Z</responseDate><request verb="GetRecord" identifier="oai:dspace.mit.edu:1721.1/79235" metadataPrefix="dim">https://dspace.mit.edu/server/oai/request</request><GetRecord><record><header><identifier>oai:dspace.mit.edu:1721.1/79235</identifier><datestamp>2022-01-13T07:54:01Z</datestamp><setSpec>com_1721.1_7582</setSpec><setSpec>com_1721.1_7581</setSpec><setSpec>col_1721.1_131023</setSpec></header><metadata><dim:dim xmlns:dim="http://www.dspace.org/xmlns/dspace/dim" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://www.dspace.org/xmlns/dspace/dim http://www.dspace.org/schema/dim.xsd">
   <dim:field mdschema="dc" element="contributor" qualifier="advisor" lang="en_US">Dennis M. Freeman.</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="author" lang="en_US">Sellon, Jonathan Blake</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="other" lang="en_US">Massachusetts Institute of Technology. Department of Electrical Engineering and Computer Science.</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="department">Massachusetts Institute of Technology. Department of Electrical Engineering and Computer Science</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="accessioned">2013-06-17T19:49:36Z</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="available">2013-06-17T19:49:36Z</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="copyright" lang="en_US">2013</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="issued" lang="en_US">2013</dim:field>
   <dim:field mdschema="dc" element="identifier" qualifier="uri">http://hdl.handle.net/1721.1/79235</dim:field>
   <dim:field mdschema="dc" element="identifier" qualifier="oclc" lang="en_US">845314459</dim:field>
   <dim:field mdschema="dc" element="description" lang="en_US">Thesis (S.M.)--Massachusetts Institute of Technology, Dept. of Electrical Engineering and Computer Science, 2013.</dim:field>
   <dim:field mdschema="dc" element="description" lang="en_US">Cataloged from PDF version of thesis.</dim:field>
   <dim:field mdschema="dc" element="description" lang="en_US">Includes bibliographical references (p. 61-64).</dim:field>
   <dim:field mdschema="dc" element="description" qualifier="abstract" lang="en_US">The tectorial membrane (TM) is thought to play a critical role in stimulating cochlear hair cells. Recently, it has been shown that the tectorial membrane supports traveling waves [14] and that these waves may contribute to cochlear tuning and sensitivity by longitudinally coupling radial cross sections [15]. While previous work examined how TM wave properties may impact a variety of hearing properties, the molecular origins controlling wave propagation are still unclear. To better understand molecular mechanisms, I examined the role of porosity and viscosity in wave propagation. Wave properties were measured for mouse TMs immersed in artificial endolymph solutions with poly-ethylene glycol (PEG) added to increase viscosity. Two PEGs with different molecular weights (MW) were used: one (8 kDa) chosen to penetrate TM pores [30] while the other (400 kDa) could not. Findings show that introducing small MW PEG increases TM wave speeds by -38% and decreases wave decay constants by -42%. Analysis of a lumped parameter model of the TM showed that these changes in wave parameters can be explained by a change in shear viscosity from ~0.2 Pa*s to ~0.65 Pa*s with no accompanying change in shear modulus. In contrast, introducing large MW PEG has little effect on wave speed (~2%) or decay (-9%), suggesting shear viscosity inside the TM is significantly more important compared to fluid viscosity. This result suggests that fluid surrounding the TM has two separate effects on TM motion. First, increasing fluid viscosity has the obvious effect of increasing drag on the surface of the TM. In addition, if high viscosity fluid penetrates the TMs porous structure then the TMs material properties are also directly affected. Of these two effects, the latter has a much greater impact on TM waves. Thus, the porosity of the TM may play a critical role in cochlear mechanics.</dim:field>
   <dim:field mdschema="dc" element="description" qualifier="statementofresponsibility" lang="en_US">by Jonathan Blake Sellon.</dim:field>
   <dim:field mdschema="dc" element="description" qualifier="degree" lang="en_US">S.M.</dim:field>
   <dim:field mdschema="dc" element="format" qualifier="extent" lang="en_US">64 p.</dim:field>
   <dim:field mdschema="dc" element="language" qualifier="iso" lang="en_US">eng</dim:field>
   <dim:field mdschema="dc" element="publisher" lang="en_US">Massachusetts Institute of Technology</dim:field>
   <dim:field mdschema="dc" element="rights" lang="en_US">M.I.T. theses are protected by 
copyright. They may be viewed from this source for any purpose, but 
reproduction or distribution in any format is prohibited without written 
permission. See provided URL for inquiries about permission.</dim:field>
   <dim:field mdschema="dc" element="rights" qualifier="uri" lang="en_US">http://dspace.mit.edu/handle/1721.1/7582</dim:field>
   <dim:field mdschema="dc" element="subject" lang="en_US">Electrical Engineering and Computer Science.</dim:field>
   <dim:field mdschema="dc" element="title" lang="en_US">Viscosity and porosity contribute to both speed and decay of tectorial membrane traveling waves</dim:field>
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   	&lt;Title>Viscosity and porosity contribute to both speed and decay of tectorial membrane traveling waves&lt;/Title>
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   	&lt;PublicationDate>2013&lt;/PublicationDate>
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        	&lt;DisplayName>Sellon, Jonathan Blake&lt;/DisplayName>
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    &lt;Keyword>Electrical Engineering and Computer Science.&lt;/Keyword>
   	&lt;Abstract>The tectorial membrane (TM) is thought to play a critical role in stimulating cochlear hair cells. Recently, it has been shown that the tectorial membrane supports traveling waves [14] and that these waves may contribute to cochlear tuning and sensitivity by longitudinally coupling radial cross sections [15]. While previous work examined how TM wave properties may impact a variety of hearing properties, the molecular origins controlling wave propagation are still unclear. To better understand molecular mechanisms, I examined the role of porosity and viscosity in wave propagation. Wave properties were measured for mouse TMs immersed in artificial endolymph solutions with poly-ethylene glycol (PEG) added to increase viscosity. Two PEGs with different molecular weights (MW) were used: one (8 kDa) chosen to penetrate TM pores [30] while the other (400 kDa) could not. Findings show that introducing small MW PEG increases TM wave speeds by -38% and decreases wave decay constants by -42%. Analysis of a lumped parameter model of the TM showed that these changes in wave parameters can be explained by a change in shear viscosity from ~0.2 Pa*s to ~0.65 Pa*s with no accompanying change in shear modulus. In contrast, introducing large MW PEG has little effect on wave speed (~2%) or decay (-9%), suggesting shear viscosity inside the TM is significantly more important compared to fluid viscosity. This result suggests that fluid surrounding the TM has two separate effects on TM motion. First, increasing fluid viscosity has the obvious effect of increasing drag on the surface of the TM. In addition, if high viscosity fluid penetrates the TMs porous structure then the TMs material properties are also directly affected. Of these two effects, the latter has a much greater impact on TM waves. Thus, the porosity of the TM may play a critical role in cochlear mechanics.&lt;/Abstract>
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