{"id":{"repo_id":"wayne-thes","oai_identifier":"oai:digitalcommons.wayne.edu:oa_dissertations-1170"},"canonical_url":"https://search.dev.ndltd.org/etd/wayne-thes/oai:digitalcommons.wayne.edu:oa_dissertations-1170","repository":{"repo_id":"wayne-thes","name":"Wayne State University","base_url":"https://digitalcommons.wayne.edu/do/oai/"},"display":{"title":"Measuring The Nanomechanics Of Nanoconfined Water Layers","abstract":"<p>Nanoconfined water has been the subject of special interest due to its applications in various fields such as biology, geology, medicine, and engineering tribology. While there is a general agreement on the layering of water molecules along atomically smooth surfaces, the behavior and properties of nanoconfined water is still poorly understood. A significant controversy exists whether there is a phase transformation imposed by confinement. We have measured the stiffness and damping coefficient of nanoconfined water using a small amplitude (0.5-1 Å) atomic force microscope. The results were analyzed with the help of two viscoelastic models, the Kelvin model and the Maxwell model. The stiffness and damping coefficient oscillate with period 2.7 ± 0.8 Å below 1 nm thickness of the water film. The retardation time and the relaxation time were measured as a function of both the strain rate and the film thickness. Above a critical strain rate, the retardation time shows valleys, and the relaxation time shows peaks commensurate with the stiffness peaks in the oscillatory profile. We call this phenomenon the Dynamic Solidification.</p> <p>The relaxation time was also measured as a function of the concentration of sodium chloride. It was found that the critical strain rate for the dynamic solidification is a function of the strength of the molarity of the solution. We found that above a critical sodium chloride concentration, water shows the dynamic solidification, even at significantly lower strain rates.</p> <p>To standardize the AFM measurements, we measured the effects of the tip size on the stiffness and damping of a nanoconfined model liquid tetrakis-2-ethyhexoxysilane (TEHOS) by using a number of tips of different sizes. We found that the stiffness and damping coefficient of the liquid increase linearly with the tip-size. We also measured an effective elastic modulus of the nanoconfined liquid and found it to be independent on the tip-size.</p>","abstract_html":"&lt;p&gt;Nanoconfined water has been the subject of special interest due to its applications in various fields such as biology, geology, medicine, and engineering tribology. While there is a general agreement on the layering of water molecules along atomically smooth surfaces, the behavior and properties of nanoconfined water is still poorly understood. A significant controversy exists whether there is a phase transformation imposed by confinement. We have measured the stiffness and damping coefficient of nanoconfined water using a small amplitude (0.5-1 Å) atomic force microscope. The results were analyzed with the help of two viscoelastic models, the Kelvin model and the Maxwell model. The stiffness and damping coefficient oscillate with period 2.7 ± 0.8 Å below 1 nm thickness of the water film. The retardation time and the relaxation time were measured as a function of both the strain rate and the film thickness. Above a critical strain rate, the retardation time shows valleys, and the relaxation time shows peaks commensurate with the stiffness peaks in the oscillatory profile. We call this phenomenon the Dynamic Solidification.&lt;/p&gt; &lt;p&gt;The relaxation time was also measured as a function of the concentration of sodium chloride. It was found that the critical strain rate for the dynamic solidification is a function of the strength of the molarity of the solution. We found that above a critical sodium chloride concentration, water shows the dynamic solidification, even at significantly lower strain rates.&lt;/p&gt; &lt;p&gt;To standardize the AFM measurements, we measured the effects of the tip size on the stiffness and damping of a nanoconfined model liquid tetrakis-2-ethyhexoxysilane (TEHOS) by using a number of tips of different sizes. We found that the stiffness and damping coefficient of the liquid increase linearly with the tip-size. We also measured an effective elastic modulus of the nanoconfined liquid and found it to be independent on the tip-size.&lt;/p&gt;","abstract_has_math":false,"creators":["Khan, Shah Haidar"],"institution":null,"degree_name":"Ph.D.","degree_level":"Open Access Dissertation","degree_discipline":"Physics and Astronomy","degree_department":null,"school":null,"contributors":["Peter M. Hoffmann"],"advisors":[],"committee_chairs":[],"committee_members":[],"year":2010,"date_issued":"2010-01-01T08:00:00Z","date_published":"2010-01-01T08:00:00Z","updated_at":"2026-07-24T05:58:42Z","subjects":["AFM","Nanoconfined Water","Condensed Matter Physics"],"languages":[],"rights":[],"rights_urls":[],"identifier_entries":[]},"links":{"outbound_url":"https://digitalcommons.wayne.edu/oa_dissertations/171","outbound_label":"Repository record","outbound_source":"dc:identifier"},"metadata_groups":[{"id":"people","label":"People","entries":[{"key":"dc:contributor","label":"Contributor","values":["Peter M. Hoffmann"]},{"key":"dc:creator","label":"Author","values":["Khan, Shah Haidar"]}]},{"id":"academic_context","label":"Academic Context","entries":[{"key":"dc:date.available","label":"Dc Date Available","values":["2011-01-04T08:00:00Z"]},{"key":"thesis:degree_discipline","label":"Discipline","values":["Physics and Astronomy"]},{"key":"thesis:degree_level","label":"Degree Level","values":["Open Access Dissertation"]},{"key":"thesis:degree_name","label":"Degree Name","values":["Ph.D."]}]},{"id":"subjects_keywords","label":"Subjects and Keywords","entries":[{"key":"dc:subject","label":"Dc Subject","values":["AFM","Nanoconfined Water","Condensed Matter Physics"]}]},{"id":"identifiers","label":"Identifiers","entries":[{"key":"dc:identifier","label":"Identifier","values":["https://digitalcommons.wayne.edu/oa_dissertations/171"]}]},{"id":"additional","label":"Additional Metadata","entries":[{"key":"dc:description.abstract","label":"Abstract","values":["<p>Nanoconfined water has been the subject of special interest due to its applications in various fields such as biology, geology, medicine, and engineering tribology. While there is a general agreement on the layering of water molecules along atomically smooth surfaces, the behavior and properties of nanoconfined water is still poorly understood. A significant controversy exists whether there is a phase transformation imposed by confinement. We have measured the stiffness and damping coefficient of nanoconfined water using a small amplitude (0.5-1 Å) atomic force microscope. The results were analyzed with the help of two viscoelastic models, the Kelvin model and the Maxwell model. The stiffness and damping coefficient oscillate with period 2.7 ± 0.8 Å below 1 nm thickness of the water film. The retardation time and the relaxation time were measured as a function of both the strain rate and the film thickness. Above a critical strain rate, the retardation time shows valleys, and the relaxation time shows peaks commensurate with the stiffness peaks in the oscillatory profile. We call this phenomenon the Dynamic Solidification.</p> <p>The relaxation time was also measured as a function of the concentration of sodium chloride. It was found that the critical strain rate for the dynamic solidification is a function of the strength of the molarity of the solution. We found that above a critical sodium chloride concentration, water shows the dynamic solidification, even at significantly lower strain rates.</p> <p>To standardize the AFM measurements, we measured the effects of the tip size on the stiffness and damping of a nanoconfined model liquid tetrakis-2-ethyhexoxysilane (TEHOS) by using a number of tips of different sizes. We found that the stiffness and damping coefficient of the liquid increase linearly with the tip-size. We also measured an effective elastic modulus of the nanoconfined liquid and found it to be independent on the tip-size.</p>"]},{"key":"dc:title","label":"Title","values":["Measuring The Nanomechanics Of Nanoconfined Water Layers"]}]}],"canonical_facts":{"dc:contributor":["Peter M. Hoffmann"],"dc:creator":["Khan, Shah Haidar"],"dc:date.available":["2011-01-04T08:00:00Z"],"dc:description.abstract":["<p>Nanoconfined water has been the subject of special interest due to its applications in various fields such as biology, geology, medicine, and engineering tribology. While there is a general agreement on the layering of water molecules along atomically smooth surfaces, the behavior and properties of nanoconfined water is still poorly understood. A significant controversy exists whether there is a phase transformation imposed by confinement. We have measured the stiffness and damping coefficient of nanoconfined water using a small amplitude (0.5-1 Å) atomic force microscope. The results were analyzed with the help of two viscoelastic models, the Kelvin model and the Maxwell model. The stiffness and damping coefficient oscillate with period 2.7 ± 0.8 Å below 1 nm thickness of the water film. The retardation time and the relaxation time were measured as a function of both the strain rate and the film thickness. Above a critical strain rate, the retardation time shows valleys, and the relaxation time shows peaks commensurate with the stiffness peaks in the oscillatory profile. We call this phenomenon the Dynamic Solidification.</p> <p>The relaxation time was also measured as a function of the concentration of sodium chloride. It was found that the critical strain rate for the dynamic solidification is a function of the strength of the molarity of the solution. We found that above a critical sodium chloride concentration, water shows the dynamic solidification, even at significantly lower strain rates.</p> <p>To standardize the AFM measurements, we measured the effects of the tip size on the stiffness and damping of a nanoconfined model liquid tetrakis-2-ethyhexoxysilane (TEHOS) by using a number of tips of different sizes. We found that the stiffness and damping coefficient of the liquid increase linearly with the tip-size. We also measured an effective elastic modulus of the nanoconfined liquid and found it to be independent on the tip-size.</p>"],"dc:identifier":["https://digitalcommons.wayne.edu/oa_dissertations/171"],"dc:subject":["AFM","Nanoconfined Water","Condensed Matter Physics"],"dc:title":["Measuring The Nanomechanics Of Nanoconfined Water Layers"],"thesis:degree_discipline":["Physics and Astronomy"],"thesis:degree_level":["Open Access Dissertation"],"thesis:degree_name":["Ph.D."]},"updated_at":"2026-07-24T05:58:42Z"}