Severity: Warning
Message: file_get_contents(https://...@pubfacts.com&api_key=b8daa3ad693db53b1410957c26c9a51b4908&a=1): Failed to open stream: HTTP request failed! HTTP/1.1 429 Too Many Requests
Filename: helpers/my_audit_helper.php
Line Number: 176
Backtrace:
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 176
Function: file_get_contents
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 250
Function: simplexml_load_file_from_url
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 3122
Function: getPubMedXML
File: /var/www/html/application/controllers/Detail.php
Line: 575
Function: pubMedSearch_Global
File: /var/www/html/application/controllers/Detail.php
Line: 489
Function: pubMedGetRelatedKeyword
File: /var/www/html/index.php
Line: 316
Function: require_once
We present a simple microscopic model describing the unique friction behavior of gecko setal arrays as they are dragged on smooth surfaces. Unlike other solids of high elastic modulus that do not stick under van der Waals forces alone, the gecko setal arrays do not require a compressive force to display a drag resistance but rather develop a tensile normal force when they are dragged (J. Experim. Biol. 2006, 209, 3569). We describe this unique behavior with a microscopic model involving curved beam structures at two length scales: at the spatula level, thousands of independent curved beams repeat detachment and reattachment, whereas at the seta level, the curved beam geometry of the seta induces a coupling between the frictional force and the adhesive force that depends on the angle of contact, therefore allowing easy release when the animal needs it. Our model accounts well for the dependence of the drag and adhesion forces on the drag velocity and can also explain macroscopic attachment/ detachment cycles of the setal array.
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Source |
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http://dx.doi.org/10.1021/jp8067415 | DOI Listing |
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