text:
@import url('https://fonts.googleapis.com/css?family=Kanit&display=swap');
font-family: 'Kanit', sans-serif;

a {
  font-family: 'Kanit', sans-serif;
}
div, h3 {
  font-Family: 'Kanit', sans-serif;
}
h1 {
  font-Family: 'Kanit', bold;
}
.header {
    animation-name: colorChange;
    animation-duration: 15s;
    animation-iteration-count: infinite;
}
@keyframes colorChange {
  0% {
      background: teal;
  }
  20% {
      background: blue;
  }
  40% {
      background: green;
  }
  60% {
      background: orange;
  }
  80% {
      background: purple;
  }
  100% {
      background: teal;
  }
}

repository: SunatP/My-web

repo_name: SunatP/My-web

gha_language: JavaScript


text:
html, body {
  margin: 0;
  padding: 0;
  min-height: 100%;
}

body {
  text-align: center;
  background: #689976;
  background: linear-gradient(#689976, #acdacc);
}

.breadcrumb {
  margin-top: 200px;
  display: inline-block;
  overflow: hidden;
  box-shadow: 0 0 15px 1px rgba(0, 0, 0, 0.35);
  border-radius: 5px;
  counter-reset: flag;
}

.breadcrumb a {
  text-decoration: none;
  outline: none;
  display: block;
  float: left;
  font-size: 12px;
  line-height: 36px;
  color: #fff;

  /* 留较宽的空白给数字 */
  padding: 0 10px 0 60px;
  background: #666;
  position: relative;

  counter: flag;
}

.breadcrumb a:first-child {
  padding-left: 46px;
  border-radius: 5px 0 0 5px;
}

.breadcrumb a:first-child:before {
  left: 14px;
}

.breadcrumb a:last-child {
  border-radius: 0 5px 5px 0;
  padding-right: 20px;
}

.breadcrumb a.active,
.breadcrumb a:hover {
  background: #333;
  background: linear-gradient(135deg, #333, #000);
}

.breadcrumb a:after {
  content: '';
  position: absolute;
  top: 0;
  right: -18px;
  width: 36px;
  height: 36px;
  transform: scale(.707) rotate(45deg);
  z-index: 1;
  background: #666;
  background: linear-gradient(135deg, #666, #333);
  box-shadow: 2px -2px 0 2px rgba(0, 0, 0, .4), 3px -3px 0 2px rgba(255, 255, 255, .1);
  border-radius: 0 5px 0 50px;
}

.breadcrumb a:last-child:after {
  content: none;
}

.breadcrumb a:before {
  content: counter(flag);
  counter-increment: flag;

  border-radius: 100%;
  width: 20px;
  height: 20px;
  line-height: 20px;
  margin: 8px 0;
  position: absolute;
  top: 0;
  left: 30px;
  background: #444;
  background: linear-gradient(#444, #222);
  font-weight: bold;
}

/* flat */
.flat a,
.flat a:after {
  background: #fff;
  color: #000;
  transition: all .5s;
}

.flat a:before {
  background: #fff;
  box-shadow: 0 0 0 1px #ccc;
}

.flat a:hover,
.flat a.active,
.flat a:hover:after,
.flat a.active:after {
  background: #9eeb62;
}

license: MIT

license_type: permissive

branch_name: refs/heads/master

extension: css


text:
#
# This file is the nbench recipe.
#

SUMMARY = "Linux/Unix nbench (previously known as BYTE's Native Mode Benchmarks)"
SECTION = "PETALINUX/apps"
#LICENSE = "nbench-byte"
#LIC_FILES_CHKSUM = "file://README;beginline=57;endline=66;md5=020ef579f8fa5746b7e307a54707834f"
LICENSE = "PD"
LIC_FILES_CHKSUM = "file://${COMMON_LICENSE_DIR}/PD;md5=b3597d12946881e13cb3b548d1173851"
SECTION = "console/utils"

# added patches from http://cgit.openembedded.org/meta-openembedded/tree/meta-oe/recipes-benchmark/nbench-byte

SRC_URI = " \
		git://github.com/Basseuph/nbench \
	  "

# file://nbench_32bits.patch
# file://Makefile-add-more-dependencies-to-pointer.h.patch

SRCREV = "98f507cc383c8d4913fd5a9c5a5a9524bb268865"

S = "${WORKDIR}"

EXTRA_OEMAKE = "-e MAKEFLAGS="

TARGET_CC_ARCH += "${CFLAGS} ${LDFLAGS}"

do_compile() {
	     oe_runmake
}

do_install() {
	     install -d ${D}${bindir}
             install -m 0644 NNET.DATA ${D}${bindir}
	     install -m 0755 nbench ${D}${bindir}
}

repository: Basseuph/ptlnx-qsim-benchmark

repo_name: Basseuph/ptlnx-qsim-benchmark

extension: bb


text:
@article{lin2018visual,
  title={Visual localizer: Outdoor localization based on convnet descriptor and global optimization for visually impaired pedestrians},
  author={Lin, Shufei and Cheng, Ruiqi and Wang, Kaiwei and Yang, Kailun},
  journal={Sensors},
  volume={18},
  number={8},
  pages={2476},
  year={2018},
  publisher={Multidisciplinary Digital Publishing Institute}
}

extension: bib


text:
@misc{Klamkin2022_ActiveBucketizedLearning,
  doi = {10.48550/ARXIV.2208.07497},
  author = {Klamkin, Michael and Tanneau, Mathieu and Mak, Terrence W. K. and Van Hentenryck, Pascal},
  title = {Active Bucketized Learning for ACOPF Optimization Proxies},
  publisher = {arXiv},
  year = {2022},
}

branch_name: refs/heads/main

gha_license_id: MIT

gha_language: TeX


text:
require pi-blaster.inc

SRCREV = "bce7c1b4c53b0dd12665e46bdebd3b7cb0987e3d"

repository: naguirre/meta-raspberrypi

repo_name: naguirre/meta-raspberrypi

gha_language: C


text:
@import 'https://fonts.googleapis.com/css?family=Open+Sans';

header{
  background: #f62459;
  width: 100%;
  height: 76px;
  position: fixed;
  top: 0;
  left:0;
  z-index: 100;
  border-bottom: 5px solid #f62459;
}

ul{
  list-style: none;
}

li{
  display: inline-block;
  float: left;
  padding:10px;
}

a{
  color:#fff;
  text-decoration: none;
  font-weight: bold;
}

a:hover{
  text-decoration: underline;
}

#logo{
  margin-left: 20px;
  float: left;
  width: 200px;
  height: 50px;
  background: url(../IMG/logo.png) no-repeat center;
  display: block;
}

nav{
  float: right;
  padding: 20px;
  font-family: 'Open Sans',sans-serif;
}

div{
  background-color: black;
  width: 32px;
  height: 5px;
  margin: 6px 0;
}

@media only screen and (max-width: 640px){
  header{
    position: absolute;
  }
  div{
    display: inline-block;
  }
  nav ul, nav:active ul{
    display: none;
    position: absolute;
    padding: 20px;
    background: #c5c5c5;
    right: 10px;
    top: 65px;
    width: 35%;
  }

  nav:hover ul{
    display: block;
  }

  nav li{
    text-align: center;
    width: 100%;
    padding: 15px 0;
    margin: 0;
  }
}

repository: albertoceballos/portfolio-Website

repo_name: albertoceballos/portfolio-Website


text:
@article{Papacharalampous-2021-Global-scale,
    title = "Global-scale massive feature extraction from monthly hydroclimatic time series: Statistical characterizations, spatial patterns and hydrological similarity",
    author = "Papacharalampous, Georgia  and
      Tyralis, Hristos  and
      Papalexiou, Simon Michael  and
      Langousis, Andreas  and
      Khatami, Sina  and
      Volpi, Elena  and
      Grimaldi, Salvatore",
    journal = "Science of The Total Environment, Volume 767",
    volume = "767",
    year = "2021",
    publisher = "Elsevier BV",
    url = "https://aclanthology.org/G21-31001",
    doi = "10.1016/j.scitotenv.2020.144612",
    pages = "144612",
}

repository: gwf-uwaterloo/gwf-publications

repo_name: gwf-uwaterloo/gwf-publications

gha_language: Python


text:
html {    overflow-y: scroll;}
body{ color:#color:#525252; border-top:solid 5px #56A4DB; background:#fff url(../img/pattern1.png);} /*background:#fff url(../img/pattern1.png);*/

/* ====== media ====== */
.media {margin:12px 0 12px 0; clear: both;}
.media, .bd {overflow:hidden; _overflow:visible; zoom:1;}
a .bd {font-size: 10px; text-decoration: none;}
.media .img {float:left; margin-right: 12px;}
.media .img img{display:block;}

.regLink { float: right; margin-right: 20px; margin-top: 3px;font-weight: bold; font-family: inherit;text-shadow: 0 1px 1px rgb(85, 85, 85); color: #fff; }
.regLink:hover { text-shadow: 0 3px 3px rgb(85, 85, 85); color: #fff; }

#login .cont, #login-collapse {width:990px;padding: 0 30px; margin:0 auto;}
.cf:before, .cf:after {content:"";display:table;}
.cf:after {clear:both;}
.cf {zoom:1;}
#login {padding-top:14px; padding-bottom: 10px;background:#56A4DB;color:#fff;text-shadow:0 0 0;font-size:13px;}
#login a {color:#0E4466;border-bottom:1px solid}
#login a:hover {color: white;}
#login p {float:left;font-size:12px;font-weight:500;padding-top: 9px;}
.ie7 #login p {display: block; float: none; width: 100%; margin-left: 380px;}
#login form {padding-top:6px;float:right; width: 600px; margin-right: 110px; }
.ie7 #login form {float: none;}
#login label {margin:0 5px 0 0; color: #0E4466; display: inline;}
#login input {margin:0 16px 0 0;padding:4px 8px; display: inline;}
#login input {background: white; text-align: left; font-size: 14px; border-width: 1px; border-style: solid; border-color: #226EB5; -moz-border-radius:4px ;-webkit-border-radius:4px; border-radius: 4px; outline: none;}
/*
#login input[type="submit"] {border:2px solid #fff;margin:0 0 0 20px;background:#45bcd2;color:#fff;text-transform:uppercase;font-size:13px;letter-spacing:1px;padding:2px 6px;}
.ie7 #login input[type="submit"] {text-align: center;padding: 2px 0 0; letter-spacing: 0;}
#login input[type="submit"]:hover {background:#0E5D86;color:#fff;}
*/

#login input[type=text], #login input[type=password] {width:150px;}

#login input.error {background-color: #FFADAD;border-color: #f40;border-width: 2px;}
#login p.sysInfo {padding-top: 4px; font-size: 14px;}

#login-collapse {text-align:center;text-shadow:0 0 0; }
#login-collapse a {position:relative;top:-4px;float:right;background:#56A4DB;color:#fff;padding:8px 20px;display:block;margin-right:15px;
    -webkit-border-radius:4px; -moz-border-radius:4px; border-radius:4px;}
#login-collapse a span {border-bottom:1px solid rgba(255,255,255,.3); border-bottom: 0;}
#login-collapse a:hover span {border-color:rgba(255,255,255,.8);}

#header{margin-top:45px; margin-bottom:60px; text-align:center;}
#header a{ display:block; width:182px; height:50px; background:url(../img/logo-fulltext.png) no-repeat center; text-indent:-9999px; margin:0 auto;}

#intro {
	background: #1373B9;
	height: 522px;
	position: relative;
	overflow: hidden;
}
#intro .background {
	position: absolute;
	top: 0;
	left: 0;
	right: 0;
	bottom: 0;
	z-index: 100;
	background-size: 100%;
	background-image: url('../../assets-home/img/nana.jpg');
	background-repeat: no-repeat;
	background-position:center;
	/* opacity: 1; */
}
#intro .wrapper {
	position: relative;
	z-index: 101;
}
#intro .wrapper {

}
.wrapper {
	width: 920px;
	margin: auto;
}

#intro .page-title-wrapper {padding-top: 100px; padding-left: 450px;}

#intro .customer-card {
	position: absolute;
	bottom: 18px;
	left: 50%;
	z-index: 102;
	margin-left: 330px;
	border-right: solid 1px rgba(255, 255, 255, 0.5);
	padding: 0px 18px;
	color: #BBB;
	font-family: "proxima-nova", sans-serif;
	line-height: 14px;
/* 	opacity: 0; */
	text-align: right;
}
#intro .customer-card h2 {
line-height: 16px;
}
#intro .customer-card h2 a {
	font-size: 11px;
	margin: 0;
	padding: 0;
	font-weight: 600;
	text-transform: uppercase;
	letter-spacing: 1px;
	color: #EEE;

}
#intro .customer-card p { 	padding-bottom: 0; margin-bottom: 0;}
#intro .customer-card p a{
	font-size: 11px;
	margin: 0;
	color:#fff;

}
#intro .customer-card a:hover { color: #005580; text-decoration: none;}

.logo {position:absolute; z-index: 106;padding-top: 40px;}

.page-title h1 { font-size:34px; font-family: 'Droid Serif', serif; font-weight: 400; margin-bottom:10px; line-height: 55px; color: #56A4DB; text-align: right;}
.page-title h1 .title-wrap {
	background-color: white;
	padding: 3px 6px;
	-ms-filter: "progid:DXImageTransform.Microsoft.Alpha(Opacity=90)";
	filter: alpha(opacity=90);
	-moz-opacity: 0.9;
	-khtml-opacity: 0.9;
	opacity: 0.9;
}
#catchycontent p{ font-size:16px; font-family: 'Droid Serif', serif; line-height:26px; font-weight:400; font-style:italic;}
#subscribe{text-align:center; margin-top:40px;}
.input-large{ padding:9px 14px; }

.btn-success {
  background-color: #d23828;
  *background-color: #d23828;
  background-image: -ms-linear-gradient(top, #d23828, #c11503);
  background-image: -webkit-gradient(linear, 0 0, 0 100%, from(#d23828), to(#c11503));
  background-image: -webkit-linear-gradient(top, #d23828, #c11503);
  background-image: -o-linear-gradient(top, #d23828, #c11503);
  background-image: -moz-linear-gradient(top, #d23828, #c11503);
  background-image: linear-gradient(top, #d23828, #c11503);
  background-repeat: repeat-x;
  border-color: #a61304 #a61304 #a61304;
  border-color: rgba(0, 0, 0, 0.1) rgba(0, 0, 0, 0.1) rgba(0, 0, 0, 0.25);
  filter: progid:dximagetransform.microsoft.gradient(startColorstr='#d23828', endColorstr='#c11503', GradientType=0);
  filter: progid:dximagetransform.microsoft.gradient(enabled=false);
}

.btn-success:hover,
.btn-success:active,
.btn-success.active,
.btn-success.disabled,
.btn-success[disabled] {
  background-color: #c11503;
  *background-color: #c11503;
}

.btn-success:active,
.btn-success.active {
  background-color: #c11503 \9;
}

.btn-large {
  padding: 9px 20px;
  font-size: 16px;
  line-height: normal;
  font-weight:700;font-family: 'Droid Serif', serif; font-style:italic;
  margin-left:10px;
  -webkit-border-radius: 5px;
     -moz-border-radius: 5px;
          border-radius: 5px;
}

input:focus,
textarea:focus {
  border-color: rgba(82, 82, 82, 0.8);
  outline: 0;
  outline: thin dotted \9;
  /* IE6-9 */

  -webkit-box-shadow: inset 0 1px 1px rgba(0, 0, 0, 0.075), 0 0 8px rgba(82, 82, 82, 0.6);
     -moz-box-shadow: inset 0 1px 1px rgba(0, 0, 0, 0.075), 0 0 8px rgba(82, 82, 82, 0.6);
          box-shadow: inset 0 1px 1px rgba(0, 0, 0, 0.075), 0 0 8px rgba(82, 82, 82, 0.6);
}

#features {margin-top:40px; text-align:center;}
.featureicon{ color:#d23828; font-size:36px; margin-bottom:15px; padding:0 20px 0 0;}
h2{ font-family: 'Droid Serif', serif; text-align:left;}
h3{ font-size:16px; font-family: 'Droid Serif', serif; line-height:26px; font-weight:700; padding:0 20px 0 0;}
#features p {font-size:12px; font-family: 'Droid Serif', serif; line-height:20px; font-weight:400;padding:0 20px 0 0;}
.divider{background:url(../img/divider.png) repeat-y right;}

.dividerHoriTop {margin-top:10px; background:url(../img/footer-divider.png) repeat-x top; padding-top:40px;}
.dividerHoriBot {margin-top:10px; background:url(../img/footer-divider.png) repeat-x bottom; padding-bottom:40px; margin-bottom: 10px;}

#footer{margin-top:20px; text-align:left; background:  url(../img/footer-divider.png) repeat-x top; padding-top:40px;}
#footer h4{ margin:0 0 20px;font-size:14px; font-family: 'Droid Serif', serif; line-height:24px; font-weight:400;}
.footericon{ color:#d23828; font-size:36px; margin-bottom:15px;margin-top: 7px;}
.footericon a{ color:#d23828;}
.footericon a:hover{ color:#a61304; text-decoration:none;}

#footer p{ font-size:10px; font-family: 'Droid Serif', serif;font-weight:400;}
#footer .media {margin-top: 0;}

.error { color: rgb(214, 18, 12); }

/* MEDIA QUERIES CUSTOM  */

@media (max-width: 480px) {
  #intro {
		height: 180px;
	}
  #intro .page-title-wrapper {
		padding-top: 40px;
		padding-left: 0px;
	}
	#login form { width: 400px; margin-right: 0px; }
	#login .cont, #login-collapse {
		width: 400px;
	}
	#login input[type=text], #login input[type=password] {width:120px;}
}

@media (max-width: 767px) {
  #intro {
		height: 300px;
	}
	.wrapper {
		width: 580px;
	}
	#intro .page-title-wrapper {
		padding-top: 40px;
		padding-left: 200px;
	}
	#intro .page-title-wrapper h1 {
		font-size: 24px;
		line-height: 38px;
	}
	#login form { width: 600px; margin-right: 0px; }
	#login .cont, #login-collapse {
		width: 500px;
	}
	#intro .customer-card {margin-left: 230px;}
	#login input[type=text], #login input[type=password] {width:120px;}
}

@media (min-width: 768px) and (max-width: 979px) {
  #intro {
		height: 430px;
	}
  .wrapper {
		width: 658px;
	}
	#intro .page-title-wrapper {
		padding-top: 90px;
		padding-left: 250px;
	}
	#intro .page-title-wrapper h1 {
		font-size: 28px;
		line-height: 46px;
	}
	#login form { width: 600px; margin-right: 0px; }
	#login .cont, #login-collapse {
		width: 753px;
	}
	#intro .customer-card {margin-left: 254px;}

	#login input[type=text], #login input[type=password] {width:150px;}
	input.span3, textarea.span3, .uneditable-input.span3 {width: 103px;}
}
@media (min-width: 1200px) {
	.wrapper {
		width: 1000px;
	}
	#login form { width: 750px; margin-right: 110px; }
	#intro .customer-card {margin-left: 380px;}
	#login input[type=text], #login input[type=password] {width:220px;}
}

@media (min-width: 1400px) {
    .logo { padding-top: 0; top:18px; }

}
@media (min-width: 1600px) {
    .logo { top:116px; left:-50px;}

}

.regLink { float: right; margin-right: 20px; margin-top: 3px;font-weight: bold; font-family: inherit;text-shadow: 0 1px 1px rgb(85, 85, 85); color: #fff; }
.regLink:hover { text-shadow: 0 3px 3px rgb(85, 85, 85); color: #fff; }

#fbLogin {
    float: right; margin-right: 20px; margin-top: 3px;
    background-image: url(/static/images/facebook_signin.png);
    width: 150px; height: 22px;
}
#fbLogin:hover {
    background-position: 0 46px;
}
#fbLogin:active {
    background-position: 0 22px;
}

repository: tanajilondhefidel/fluxtream-app-master

repo_name: tanajilondhefidel/fluxtream-app-master


text:
SUMMARY = "Phosphor OpenBMC IPMI daemon"
DESCRIPTION = "Phosphor OpenBMC IPMI router and plugin libraries"
HOMEPAGE = "http://github.com/openbmc/phosphor-host-ipmid"
PR = "r1"

inherit obmc-phosphor-license
inherit obmc-phosphor-systemd

DEPENDS += "glib-2.0"
SRC_URI += "git://github.com/openbmc/phosphor-host-ipmid"

SRCREV = "02d37aab090090af9a779f4039931a6721bff615"

S = "${WORKDIR}/git"

do_install() {
        install -m 0755 -d ${D}${sbindir} ${D}${libdir} ${D}${libdir}/host-ipmid/
        install -m 0755 ${S}/ipmid ${D}${sbindir}/
        install -m 0755 ${S}/libapphandler.so ${D}${libdir}/host-ipmid/
}

repository: jk-ozlabs/openbmc

repo_name: jk-ozlabs/openbmc


text:
DESCRIPTION = "OPKG Package Manager Utilities"
SECTION = "base"
HOMEPAGE = "http://wiki.openmoko.org/wiki/Opkg"
PRIORITY = "optional"
RDEPENDS_${PN} = "python"
RDEPENDS_${PN}_virtclass-native = ""

GITREV = "16665959c330b5958c0f0f4624a9ca7f823f98de"
PV = "0.1.8+git-${GITREV}"
PR = "r8"

#SRC_URI = "git://git.yoctoproject.org/opkg-utils;protocol=git"
SRC_URI = "http://git.yoctoproject.org/cgit/cgit.cgi/opkg-utils/snapshot/opkg-utils-${GITREV}.tar.gz \
	    file://index-ignore-filenotfound.patch \
	    file://mtime-int.patch"

S = "${WORKDIR}/opkg-utils-${GITREV}"

# Avoid circular dependencies from package_ipk.bbclass
PACKAGES_virtclass-native = ""

do_install() {
        oe_runmake PREFIX=${prefix} DESTDIR=${D} install
}

BBCLASSEXTEND = "native"
TARGET_CC_ARCH += "${LDFLAGS}"


text:
# base recipe: meta/recipes-extended/ethtool/ethtool_4.19.bb
# base branch: warrior
# base commit: c8c383d958807b991e31d22f612ba2a81a3860a4

FILESPATH_append = ":${COREBASE}/meta/recipes-extended/ethtool/ethtool"
SUMMARY = "Display or change ethernet card settings"
DESCRIPTION = "A small utility for examining and tuning the settings of your ethernet-based network interfaces."
HOMEPAGE = "http://www.kernel.org/pub/software/network/ethtool/"
SECTION = "console/network"
LICENSE = "GPLv2+"
LIC_FILES_CHKSUM = "file://COPYING;md5=b234ee4d69f5fce4486a80fdaf4a4263 \
                    file://ethtool.c;beginline=4;endline=17;md5=c19b30548c582577fc6b443626fc1216"

inherit autotools ptest
inherit debian-package
require recipes-debian/sources/ethtool.inc

SRC_URI += " \
           file://run-ptest \
           file://avoid_parallel_tests.patch \
           "

RDEPENDS_${PN}-ptest += "make"

do_compile_ptest() {
   oe_runmake buildtest-TESTS
}

do_install_ptest () {
   cp ${B}/Makefile                 ${D}${PTEST_PATH}
   install ${B}/test-cmdline        ${D}${PTEST_PATH}
   install ${B}/test-features       ${D}${PTEST_PATH}
   install ${B}/ethtool             ${D}${PTEST_PATH}/ethtool
   sed -i 's/^Makefile/_Makefile/'  ${D}${PTEST_PATH}/Makefile
}

repository: miraclelinux/meta-debian-extended

repo_name: miraclelinux/meta-debian-extended

branch_name: refs/heads/warrior

gha_language: BitBake


text:
@inproceedings{ECDLEerola2005,
  author       = {Johanna Eerola and Pertti Vakkari},
  title        = {How a general and a specific thesaurus covers expressions in patients' questions and physicians' answers},
  year = {2005},
  venue        = {European Conference on Digital Libraries},
  location     = {Vienna, Austria},
  url={https://web.archive.org/web/20110412154648/http://www2.db.dk/nkos2005/Eerola%20-%20Vikkari.pdf}
}

@inproceedings{ECDLSanatjoo2005,
  author       = {Azam Sanatjoo},
  title        = {User's perception with work task oriented thesaurus design},
  year = {2005},
  venue        = {European Conference on Digital Libraries},
  location     = {Vienna, Austria},
  url={https://web.archive.org/web/20110412154648/http://www2.db.dk/nkos2005/Azam%20Sanatjoo.pdf}
}

@inproceedings{ECDLNielsen2005,
  author       = {Marianne Lykke Nielsen and Mathew J. Weaver and Lois Delcambre and Timothy Tolle},
  title        = {Enhancing domain-specific digital library with facilities for vocabulary exploration},
  year = {2005},
  venue        = {European Conference on Digital Libraries},
  location     = {Vienna, Austria},
  url={https://web.archive.org/web/20110412154648/http://www2.db.dk/nkos2005/Nielsen_Weaver_mfl.pdf}
}

@inproceedings{ECDLDavies2005,
  author       = {Ron Davies},
  title        = {Case study on agency-wide taxonomy for intergovernmental organization},
  year = {2005},
  venue        = {European Conference on Digital Libraries},
  location     = {Vienna, Austria},
 }

@inproceedings{ECDLAlistairMiles2005,
  author       = {Alistair Miles and Brian Mattews and Michael Wilson and Dan Brickley},
  title        = {NKOS issues in W3C's Simple Knowledge Organisation System (SKOS)},
  year = {2005},
  venue        = {European Conference on Digital Libraries},
  location     = {Vienna, Austria},
  url={https://web.archive.org/web/20110412154648/http://www2.db.dk/nkos2005/miles_matthews_wilson.pdf}
}

@inproceedings{ECDLMargheritaSini2005,
  author       = {Margherita Sini},
  title        = {The specification of a mapping schema linking the Chinese agricultural thesaurus to AGROVOC},
  year = {2005},
  venue        = {European Conference on Digital Libraries},
  location     = {Vienna, Austria},
  url={https://web.archive.org/web/20110412154648/http://www2.db.dk/nkos2005/Margherita%20Sini.pdf}
}

@inproceedings{ECDLRJBater2005,
  author       = {R J Bater},
  title        = {Third order knowledge mapping},
  year = {2005},
  venue        = {European Conference on Digital Libraries},
  location     = {Vienna, Austria},
  url={https://web.archive.org/web/20110412154648/http://www2.db.dk/nkos2005/Bob%20Bater.pdf}
}

@inproceedings{ECDLPeterScheir2005,
  author       = {Peter Scheir and Stefanie Lindstaedt and Mathias Lux},
  title        = {Associative retrieval over different knowledge organization systems},
  year = {2005},
  venue        = {European Conference on Digital Libraries},
  location     = {Vienna, Austria},
  url={https://web.archive.org/web/20110412154648/http://www2.db.dk/nkos2005/Scheir_Lux_Lindstaedt.pdf}
}

@inproceedings{ECDLClarke2005,
  author       = {Stella Dextre Clarke},
  title        = {Revision and extension of thesaurus standards},
  year = {2005},
  venue        = {European Conference on Digital Libraries},
  location     = {Vienna, Austria},
  url={https://web.archive.org/web/20110412154648/http://www2.db.dk/nkos2005/Stella_Dextre_Clarke.pdf}
}

@inproceedings{ECDLEdwardAFox2005,
  author       = {Edward Fox and Baoping Zhang and Ryan Richardson},
  title        = {Networked knowledge organization for the networked digital library of theses and dissertations},
  year = {2005},
  venue        = {European Conference on Digital Libraries},
  location     = {Vienna, Austria},
  url={https://web.archive.org/web/20110412154648/http://www2.db.dk/nkos2005/Fox-Zhang-Richardson.pdf}
}

@inproceedings{ECDLCassel2005,
  author       = {Lillian Cassel},
  title        = {Supporting the development of the union of computing disciplines},
  year = {2005},
  venue        = {European Conference on Digital Libraries},
  location     = {Vienna, Austria},
  url={https://web.archive.org/web/20110412154648/http://www2.db.dk/nkos2005/Boots%20Cassel.pdf}
}

@inproceedings{ECDLFalquet2005,
  author       = {Gilles Falquet and Luka Nerima and Claire-Lise Mottaz Jiang and Jean-Claude Ziswiler},
  title        = {Building virtual documents by integrating hyperbooks},
  year = {2005},
  venue        = {European Conference on Digital Libraries},
  location     = {Vienna, Austria},
  url={https://web.archive.org/web/20110412154648/http://www2.db.dk/nkos2005/Ziswiler.pdf}
}

repository: PhilippMayr/NKOS-bibliography

repo_name: PhilippMayr/NKOS-bibliography


text:
configure_file(javascriptcoregtk.pc.in ${CMAKE_BINARY_DIR}/Source/JavaScriptCore/javascriptcoregtk-${WEBKITGTK_API_VERSION}.pc @ONLY)
configure_file(JavaScriptCore.gir.in ${CMAKE_BINARY_DIR}/JavaScriptCore-${WEBKITGTK_API_VERSION}.gir @ONLY)

add_custom_command(
    OUTPUT ${CMAKE_BINARY_DIR}/JavaScriptCore-${WEBKITGTK_API_VERSION}.typelib
    DEPENDS ${CMAKE_BINARY_DIR}/JavaScriptCore-${WEBKITGTK_API_VERSION}.gir
    COMMAND ${INTROSPECTION_COMPILER} ${CMAKE_BINARY_DIR}/JavaScriptCore-${WEBKITGTK_API_VERSION}.gir -o ${CMAKE_BINARY_DIR}/JavaScriptCore-${WEBKITGTK_API_VERSION}.typelib
)

ADD_TYPELIB(${CMAKE_BINARY_DIR}/JavaScriptCore-${WEBKITGTK_API_VERSION}.typelib)

install(FILES "${CMAKE_BINARY_DIR}/Source/JavaScriptCore/javascriptcoregtk-${WEBKITGTK_API_VERSION}.pc"
        DESTINATION "${LIB_INSTALL_DIR}/pkgconfig"
)

install(FILES API/JavaScript.h
              API/JSBase.h
              API/JSContextRef.h
              API/JSObjectRef.h
              API/JSStringRef.h
              API/JSValueRef.h
              API/WebKitAvailability.h
        DESTINATION "${WEBKITGTK_HEADER_INSTALL_DIR}/JavaScriptCore"
)

install(FILES ${CMAKE_BINARY_DIR}/JavaScriptCore-${WEBKITGTK_API_VERSION}.gir
        DESTINATION ${INTROSPECTION_INSTALL_GIRDIR}
)
install(FILES ${CMAKE_BINARY_DIR}/JavaScriptCore-${WEBKITGTK_API_VERSION}.typelib
        DESTINATION ${INTROSPECTION_INSTALL_TYPELIBDIR}
)

repository: adzhou/oragle

repo_name: adzhou/oragle

extension: cmake


text:
@article{fernandez-toledano_contact-line_2019,
	title = {Contact-line fluctuations and dynamic wetting},
	volume = {540},
	issn = {0021-9797},
	url = {http://www.sciencedirect.com/science/article/pii/S0021979719300402},
	doi = {10.1016/j.jcis.2019.01.041},
	abstract = {Hypothesis
The thermal fluctuations of the three-phase contact line formed between a liquid and a solid at equilibrium can be used to determine key parameters that control dynamic wetting.
Methods
We use large-scale molecular dynamics simulations and Lennard-Jones potentials to model a liquid bridge between two molecularly smooth solid surfaces and study the positional fluctuations of the contact lines so formed as a function of the solid–liquid interaction.
Findings
We show that the fluctuations have a Gaussian distribution and may be modelled as an overdamped one-dimensional Langevin oscillator. Our analysis allows us to extract the coefficients of friction per unit length of the contact lines ζ, which arise from the collective interaction of the contact-line’s constituent liquid atoms with each other and the solid surface. We then compare these coefficients with those obtained by measuring the dynamic contact angle as a function of contact-line speed in independent simulations and applying the molecular-kinetic theory of dynamic wetting. We find excellent agreement between the two, with the same dependence on solid–liquid interaction and, therefore, the equilibrium contact angle θ0. As well as providing further evidence for the underlying validity of the molecular-kinetic model, our results suggest that it should be possible to predict the dynamics of wetting and, in particular, the velocity-dependence of the local, microscopic dynamic contact angle, by experimentally measuring the fluctuations of the contact line of a capillary system at equilibrium. This would circumvent the need to measure the microscopic dynamic contact angle directly.},
	language = {en},
	urldate = {2020-08-03},
	journal = {Journal of Colloid and Interface Science},
	author = {Fernández-Toledano, J-C. and Blake, T. D. and De Coninck, J.},
	month = mar,
	year = {2019},
	keywords = {Contact angles, Langevin process, Molecular-dynamics, Molecular-kinetic theory, Solid–liquid interactions},
	pages = {322--329},
	file = {ScienceDirect Snapshot:/home/u1996721/Zotero/storage/A9QVA5PM/S0021979719300402.html:text/html;ScienceDirect Full Text PDF:/home/u1996721/Zotero/storage/79A6Y5X2/Fernández-Toledano et al. - 2019 - Contact-line fluctuations and dynamic wetting.pdf:application/pdf}
}

@article{blake_forced_2015,
	title = {Forced wetting and hydrodynamic assist},
	volume = {27},
	issn = {1070-6631},
	url = {https://0-aip-scitation-org.pugwash.lib.warwick.ac.uk/doi/full/10.1063/1.4934703},
	doi = {10.1063/1.4934703},
	abstract = {Wetting is a prerequisite for coating a uniform layer of liquid onto a solid. Wetting failure and air entrainment set the ultimate limit to coating speed. It is well known in the coating art that this limit can be postponed by manipulating the coating flow to generate what has been termed “hydrodynamic assist,” but the underlying mechanism is unclear. Experiments have shown that the conditions that postpone air entrainment also reduce the apparent dynamic contact angle, suggesting a direct link, but how the flow might affect the contact angle remains to be established. Here, we use molecular dynamics to compare the outcome of steady forced wetting with previous results for the spontaneous spreading of liquid drops and apply the molecular-kinetic theory of dynamic wetting to rationalize our findings and place them on a quantitative footing. The forced wetting simulations reveal significant slip at the solid-liquid interface and details of the flow immediately adjacent to the moving contact line. Our results confirm that the local, microscopic contact angle is dependent not simply only on the velocity of wetting but also on the nature of the flow that drives it. In particular, they support an earlier suggestion that during forced wetting, an intense shear stress in the vicinity of the contact line can assist surface tension forces in promoting dynamic wetting, thus reducing the velocity-dependence of the contact angle. Hydrodynamic assist then appears as a natural consequence of wetting that emerges when the contact line is driven by a strong and highly confined flow. Our theoretical approach also provides a self-consistent model of molecular slip at the solid-liquid interface that enables its magnitude to be estimated from dynamic contact angle measurements. In addition, the model predicts how hydrodynamic assist and slip may be influenced by liquid viscosity and solid-liquid interactions.},
	number = {11},
	urldate = {2020-08-04},
	journal = {Physics of Fluids},
	author = {Blake, Terence D. and Fernandez-Toledano, Juan-Carlos and Doyen, Guillaume and De Coninck, Joël},
	month = nov,
	year = {2015},
	note = {Publisher: American Institute of Physics},
	pages = {112101},
	file = {Full Text PDF:/home/u1996721/Zotero/storage/GD4SC7WB/Blake et al. - 2015 - Forced wetting and hydrodynamic assist.pdf:application/pdf;Snapshot:/home/u1996721/Zotero/storage/LIJL8B84/1.html:text/html}
}

@article{zhao_revisiting_2019,
	title = {Revisiting the {Rayleigh}–{Plateau} instability for the nanoscale},
	volume = {861},
	issn = {0022-1120, 1469-7645},
	url = {https://www.cambridge.org/core/journals/journal-of-fluid-mechanics/article/revisiting-the-rayleighplateau-instability-for-the-nanoscale/3E1DF0F54F5C3BE949F510284A5F82DA},
	doi = {10.1017/jfm.2018.950},
	abstract = {The theoretical framework developed by Rayleigh and Plateau in the 19th century has been remarkably accurate in describing macroscale experiments of liquid cylinder instability. Here we re-evaluate and revise the Rayleigh–Plateau instability for the nanoscale, where molecular dynamics experiments demonstrate its inadequacy. A new framework based on the stochastic lubrication equation is developed that captures nanoscale flow features and highlights the critical role of thermal fluctuations at small scales. Remarkably, the model indicates that classically stable (i.e. ‘fat’) liquid cylinders can be broken at the nanoscale, and this is confirmed by molecular dynamics.},
	language = {en},
	urldate = {2020-08-04},
	journal = {Journal of Fluid Mechanics},
	author = {Zhao, Chengxi and Sprittles, James E. and Lockerby, Duncan A.},
	month = feb,
	year = {2019},
	note = {Publisher: Cambridge University Press},
	keywords = {breakup/coalescence, capillary flows, non-continuum effects},
	file = {Full Text PDF:/home/u1996721/Zotero/storage/DL4BLCZU/Zhao et al. - 2019 - Revisiting the Rayleigh–Plateau instability for th.pdf:application/pdf;Snapshot:/home/u1996721/Zotero/storage/JRAZZIKS/3E1DF0F54F5C3BE949F510284A5F82DA.html:text/html}
}

@article{zhang_molecular_2019,
	title = {Molecular simulation of thin liquid films: {Thermal} fluctuations and instability},
	volume = {100},
	shorttitle = {Molecular simulation of thin liquid films},
	url = {https://link.aps.org/doi/10.1103/PhysRevE.100.023108},
	doi = {10.1103/PhysRevE.100.023108},
	abstract = {The instability of a thin liquid film on a solid surface is studied both by molecular dynamics simulations (MD) and a stochastic thin-film equation (STF), which models thermal fluctuations with white noise. A linear stability analysis of the STF allows us to derive a power spectrum for the surface fluctuations, which is quantitatively validated against the spectrum observed in MD. Thermal fluctuations are shown to be critical to the dynamics of nanoscale films. Compared to the classical instability mechanism, which is driven by disjoining pressure, fluctuations (a) can massively amplify the instability, (b) cause the fluctuation wavelength that is dominant to evolve in time (a single fastest-growing mode does not exist), and (c) decrease the critical wavelength so that classically stable films can be ruptured.},
	number = {2},
	urldate = {2020-08-04},
	journal = {Physical Review E},
	author = {Zhang, Yixin and Sprittles, James E. and Lockerby, Duncan A.},
	month = aug,
	year = {2019},
	note = {Publisher: American Physical Society},
	pages = {023108},
	file = {Full Text PDF:/home/u1996721/Zotero/storage/68F4I28Y/Zhang et al. - 2019 - Molecular simulation of thin liquid films Thermal.pdf:application/pdf;APS Snapshot:/home/u1996721/Zotero/storage/YM9E25NX/PhysRevE.100.html:text/html}
}

@article{plimpton_fast_1995,
	title = {Fast {Parallel} {Algorithms} for {Short}-{Range} {Molecular} {Dynamics}},
	volume = {117},
	issn = {0021-9991},
	url = {http://www.sciencedirect.com/science/article/pii/S002199918571039X},
	doi = {10.1006/jcph.1995.1039},
	abstract = {Three parallel algorithms for classical molecular dynamics are presented. The first assigns each processor a fixed subset of atoms; the second assigns each a fixed subset of inter-atomic forces to compute; the third assigns each a fixed spatial region. The algorithms are suitable for molecular dynamics models which can be difficult to parallelize efficiently—those with short-range forces where the neighbors of each atom change rapidly. They can be implemented on any distributed-memory parallel machine which allows for message-passing of data between independently executing processors. The algorithms are tested on a standard Lennard-Jones benchmark problem for system sizes ranging from 500 to 100,000,000 atoms on several parallel supercomputers--the nCUBE 2, Intel iPSC/860 and Paragon, and Cray T3D. Comparing the results to the fastest reported vectorized Cray Y-MP and C90 algorithm shows that the current generation of parallel machines is competitive with conventional vector supercomputers even for small problems. For large problems, the spatial algorithm achieves parallel efficiencies of 90\% and a 1840-node Intel Paragon performs up to 165 faster than a single Cray C9O processor. Trade-offs between the three algorithms and guidelines for adapting them to more complex molecular dynamics simulations are also discussed.},
	language = {en},
	number = {1},
	urldate = {2020-08-04},
	journal = {Journal of Computational Physics},
	author = {Plimpton, Steve},
	month = mar,
	year = {1995},
	pages = {1--19},
	file = {ScienceDirect Snapshot:/home/u1996721/Zotero/storage/QIM33W2X/S002199918571039X.html:text/html;ScienceDirect Full Text PDF:/home/u1996721/Zotero/storage/Q4TEQ2GD/Plimpton - 1995 - Fast Parallel Algorithms for Short-Range Molecular.pdf:application/pdf}
}

@article{trokhymchuk_computer_1999,
	title = {Computer simulations of liquid/vapor interface in {Lennard}-{Jones} fluids: {Some} questions and answers},
	volume = {111},
	issn = {0021-9606},
	shorttitle = {Computer simulations of liquid/vapor interface in {Lennard}-{Jones} fluids},
	url = {https://0-aip-scitation-org.pugwash.lib.warwick.ac.uk/doi/10.1063/1.480192},
	doi = {10.1063/1.480192},
	number = {18},
	urldate = {2020-08-04},
	journal = {The Journal of Chemical Physics},
	author = {Trokhymchuk, Andrij and Alejandre, José},
	month = oct,
	year = {1999},
	note = {Publisher: American Institute of Physics},
	pages = {8510--8523},
	file = {Full Text PDF:/home/u1996721/Zotero/storage/KC5U8QYQ/Trokhymchuk and Alejandre - 1999 - Computer simulations of liquidvapor interface in .pdf:application/pdf;Snapshot:/home/u1996721/Zotero/storage/ZIUSLAL4/1.html:text/html}
}

@article{haile_molecular_1993,
	title = {Molecular {Dynamics} {Simulation}: {Elementary} {Methods}},
	volume = {7},
	issn = {0894-1866},
	shorttitle = {Molecular {Dynamics} {Simulation}},
	url = {https://aip.scitation.org/doi/10.1063/1.4823234},
	doi = {10.1063/1.4823234},
	number = {6},
	urldate = {2020-08-04},
	journal = {Computers in Physics},
	author = {Haile, J. M. and Johnston, Ian and Mallinckrodt, A. John and McKay, Susan},
	month = nov,
	year = {1993},
	note = {Publisher: American Institute of Physics},
	pages = {625--625},
	file = {Full Text PDF:/home/u1996721/Zotero/storage/FVQUYTBN/Haile et al. - 1993 - Molecular Dynamics Simulation Elementary Methods.pdf:application/pdf;Snapshot:/home/u1996721/Zotero/storage/47IMG6QI/1.html:text/html}
}

@article{smith_langevin_2016,
	title = {A {Langevin} model for fluctuating contact angle behaviour parametrised using molecular dynamics},
	volume = {12},
	issn = {1744-6848},
	url = {http://0.pubs.rsc.org/en/content/articlelanding/2016/sm/c6sm01980c},
	doi = {10.1039/C6SM01980C},
	abstract = {Molecular dynamics simulations are employed to develop a theoretical model to predict the fluid–solid contact angle as a function of wall-sliding speed incorporating thermal fluctuations. A liquid bridge between counter-sliding walls is studied, with liquid–vapour interface-tracking, to explore the impact of wall-sliding speed on contact angle. The behaviour of the macroscopic contact angle varies linearly over a range of capillary numbers beyond which the liquid bridge pinches off, a behaviour supported by experimental results. Nonetheless, the liquid bridge provides an ideal test case to study molecular scale thermal fluctuations, which are shown to be well described by Gaussian distributions. A Langevin model for contact angle is parametrised to incorporate the mean, fluctuation and auto-correlations over a range of sliding speeds and temperatures. The resulting equations can be used as a proxy for the fully-detailed molecular dynamics simulation allowing them to be integrated within a continuum-scale solver.},
	language = {en},
	number = {48},
	urldate = {2020-08-04},
	journal = {Soft Matter},
	author = {Smith, E. R. and Müller, E. A. and Craster, R. V. and Matar, O. K.},
	month = dec,
	year = {2016},
	note = {Publisher: The Royal Society of Chemistry},
	pages = {9604--9615},
	file = {Full Text PDF:/home/u1996721/Zotero/storage/PN5LI9IQ/Smith et al. - 2016 - A Langevin model for fluctuating contact angle beh.pdf:application/pdf;Snapshot:/home/u1996721/Zotero/storage/F32NMKCQ/unauth.html:text/html}
}

@article{blake_contact_1997,
	title = {Contact {Angle} {Relaxation} during {Droplet} {Spreading}:  {Comparison} between {Molecular} {Kinetic} {Theory} and {Molecular} {Dynamics}},
	volume = {13},
	issn = {0743-7463},
	shorttitle = {Contact {Angle} {Relaxation} during {Droplet} {Spreading}},
	url = {http://0.doi.org/10.1021/la962004g},
	doi = {10.1021/la962004g},
	abstract = {The macroscopic behavior of the contact line during the spontaneous spreading of a droplet can be described in terms of microscopic quantities, specifically the substrate−liquid and liquid−liquid interactions. Here, for the first time, the results of molecular dynamics simulations of very large sessile drop systems are compared with the predictions of the molecular−kinetic theory of wetting. Good agreement is obtained, with both approaches yielding a consistent set of molecular parameters and macroscopic behavior which is consistent with experiments.},
	number = {7},
	urldate = {2020-08-04},
	journal = {Langmuir},
	author = {Blake, T. D. and Clarke, A. and De Coninck, J. and de Ruijter, M. J.},
	month = apr,
	year = {1997},
	note = {Publisher: American Chemical Society},
	pages = {2164--2166},
	file = {Full Text PDF:/home/u1996721/Zotero/storage/RMEZ6QF4/Blake et al. - 1997 - Contact Angle Relaxation during Droplet Spreading.pdf:application/pdf;ACS Full Text Snapshot:/home/u1996721/Zotero/storage/VZ4C2DZI/la962004g.html:text/html}
}

@article{ramer_iterative_1972,
	title = {An iterative procedure for the polygonal approximation of plane curves},
	volume = {1},
	issn = {0146-664X},
	url = {http://www.sciencedirect.com/science/article/pii/S0146664X72800170},
	doi = {10.1016/S0146-664X(72)80017-0},
	abstract = {The approximation of arbitrary two-dimensional curves by polygons is an importanttechnique in image processing. For many applications, the apparent ideal procedure is to represent lines and boundaries by means of polygons with minimum number of vertices and satisfying a given fit criterion. In this paper, an approximation algorithm is presented which uses an iterative method to produce polygons with a small—but not minimum—number of vertices that lie on the given curve. The maximum distance of the curve from the approximating polygon is chosen as the fit criterion. The results obtained justify the abandonment of the minimum-vertices criterion which is computationally much more expensive.},
	language = {en},
	number = {3},
	urldate = {2020-08-09},
	journal = {Computer Graphics and Image Processing},
	author = {Ramer, Urs},
	month = nov,
	year = {1972},
	pages = {244--256},
	file = {ScienceDirect Snapshot:/home/u1996721/Zotero/storage/3XYQXAFF/S0146664X72800170.html:text/html;ScienceDirect Full Text PDF:/home/u1996721/Zotero/storage/8ITUZVBW/Ramer - 1972 - An iterative procedure for the polygonal approxima.pdf:application/pdf}
}

@article{feldman_theory_1989,
	title = {The theory of polymer dynamics, by {M}. {Doi} and {S}. {F}. {Edwards}, the {Clarendon} {Press}, {Oxford} {University} {Press}, {New} {York}, 1986, 391 pp. {Price}: \$78.50.},
	volume = {27},
	issn = {0887-6258},
	shorttitle = {The theory of polymer dynamics, by {M}. {Doi} and {S}. {F}. {Edwards}, the {Clarendon} {Press}, {Oxford} {University} {Press}, {New} {York}, 1986, 391 pp. {Price}},
	url = {https://0-onlinelibrary-wiley-com.pugwash.lib.warwick.ac.uk/doi/abs/10.1002/pol.1989.140270706},
	doi = {10.1002/pol.1989.140270706},
	number = {7},
	urldate = {2020-08-09},
	journal = {Journal of Polymer Science Part C: Polymer Letters},
	author = {Feldman, D.},
	month = jun,
	year = {1989},
	note = {Publisher: John Wiley \& Sons, Ltd},
	pages = {239--240},
	file = {Snapshot:/home/u1996721/Zotero/storage/GUGNCHWA/pol.1989.html:text/html}
}

@article{lax_fluctuations_1960,
	title = {Fluctuations from the {Nonequilibrium} {Steady} {State}},
	volume = {32},
	url = {https://link.aps.org/doi/10.1103/RevModPhys.32.25},
	doi = {10.1103/RevModPhys.32.25},
	abstract = {DOI:https://doi.org/10.1103/RevModPhys.32.25},
	number = {1},
	urldate = {2020-08-09},
	journal = {Reviews of Modern Physics},
	author = {Lax, Melvin},
	month = jan,
	year = {1960},
	note = {Publisher: American Physical Society},
	pages = {25--64},
	file = {APS Snapshot:/home/u1996721/Zotero/storage/8LSPPATS/RevModPhys.32.html:text/html}
}

@article{lax_classical_1966,
	title = {Classical {Noise} {IV}: {Langevin} {Methods}},
	volume = {38},
	shorttitle = {Classical {Noise} {IV}},
	url = {http://0.link.aps.org/doi/10.1103/RevModPhys.38.541},
	doi = {10.1103/RevModPhys.38.541},
	abstract = {A Langevin theory for linear and nonlinear, stationary and nonstationary, processes is developed and compared with Markoff methods. For short correlation times τc, we find the Markoff process that is a good approximation to the Langevin process for Δt{\textgreater}τc. Conversely, given the diffusion coefficients Dn of a Markoff process, we find the moments (to all orders) of the Langevin forces that lead to the same process—exactly for homogeneous noise, approximately for the general nonlinear case. The techniques are illustrated by applications to Fokker-Planck processes, homogeneous noise with linear damping, the one-dimensional impurity band, spin diffusion, and population fluctuations.},
	number = {3},
	urldate = {2020-08-09},
	journal = {Reviews of Modern Physics},
	author = {LAX, MELVIN},
	month = jul,
	year = {1966},
	note = {Publisher: American Physical Society},
	pages = {541--566},
	file = {Full Text PDF:/home/u1996721/Zotero/storage/9QUAYJPG/LAX - 1966 - Classical Noise IV Langevin Methods.pdf:application/pdf;APS Snapshot:/home/u1996721/Zotero/storage/HB75Z584/RevModPhys.38.html:text/html}
}

@article{abraham_langevin_1990,
	title = {Langevin dynamics of an interface near a wall},
	volume = {61},
	copyright = {1990 Plenum Publishing Corporation},
	issn = {1572-9613},
	url = {https://0-link-springer-com.pugwash.lib.warwick.ac.uk/article/10.1007/BF01027290},
	doi = {10.1007/BF01027290},
	abstract = {We study dynamical contact angles and precursor films using Langevin dynamics for SOS type models, near a wall which favors spreading. We first solve exactly the Gaussian model and discuss various asymptotic regimes. This is only appropriate to partial wetting. We then consider more general models. Using local equilibrium and scaling arguments, we derive the shape of the dynamical profile and the speed of the precursor film which exists when the spreading coefficient is strictly positive. Long-range potentials lead to a layered structure of the precursor film. We also consider the case of a meniscus in a capillary.},
	language = {en},
	number = {3},
	urldate = {2020-08-11},
	journal = {Journal of Statistical Physics},
	author = {Abraham, Douglas and Collet, Pierre and Coninck, Joël De and Dunlop, Fran/ccois},
	month = nov,
	year = {1990},
	note = {Company: Springer
Distributor: Springer
Institution: Springer
Label: Springer
Number: 3
Publisher: Kluwer Academic Publishers-Plenum Publishers},
	pages = {509--532},
	file = {Full Text PDF:/home/u1996721/Zotero/storage/ZM8PVMB2/Abraham et al. - 1990 - Langevin dynamics of an interface near a wall.pdf:application/pdf;Snapshot:/home/u1996721/Zotero/storage/7A4LA9DQ/10.html:text/html}
}

@article{voue_spreading_2000,
	title = {Spreading and wetting at the microscopic scale: recent developments and perspectives},
	volume = {48},
	issn = {1359-6454},
	shorttitle = {Spreading and wetting at the microscopic scale},
	url = {http://www.sciencedirect.com/science/article/pii/S1359645400002275},
	doi = {10.1016/S1359-6454(00)00227-5},
	abstract = {In both the experimental and numerical approaches of wettability, the spreading phenomenon is now understood as the consequence of the competition between a driving term (i.e. the affinity of the liquid for the solid) and the friction of the liquid molecules on the substrate. The aim of this article is to review how the combination of molecular dynamics (MD) simulations and of microscopic scale experiments leads to a better understanding of the physico-chemical properties of the solid/liquid interface and to present the most recent developments achieved in the complete wetting regime.},
	language = {en},
	number = {18},
	urldate = {2020-08-11},
	journal = {Acta Materialia},
	author = {Voué, M. and De Coninck, J.},
	month = dec,
	year = {2000},
	keywords = {Coating, Computer simulation, Interface, Liquids, Surfaces},
	pages = {4405--4417},
	file = {ScienceDirect Snapshot:/home/u1996721/Zotero/storage/ZDTXGYNN/S1359645400002275.html:text/html;ScienceDirect Full Text PDF:/home/u1996721/Zotero/storage/E79TXAR5/Voué and De Coninck - 2000 - Spreading and wetting at the microscopic scale re.pdf:application/pdf}
}

@article{huh_hydrodynamic_1971,
	title = {Hydrodynamic model of steady movement of a solid/liquid/fluid contact line},
	volume = {35},
	issn = {0021-9797},
	url = {http://www.sciencedirect.com/science/article/pii/0021979771901883},
	doi = {10.1016/0021-9797(71)90188-3},
	abstract = {Movement of the contact line over a solid surface violates the adherence, or “no slip,” boundary condition which is otherwise obeyed by flowing liquids. A flat fluid interface moving steadily over a flat solid is modeled with the creeping flow approximation, which turns out to be self-consistent. Adherence is required except at the contact line itself. Though the velocity field appears to be realistic, stresses and viscous dissipation are found to increase without bound at the contact line. The way the hydrodynamic model breaks down suggests that in reality there may be steep gradients, rheological anomalies, and discontinuous processes around the contact line. Slip and the role of long-range forces are explored with the aid of the lubrication flow approximation.},
	language = {en},
	number = {1},
	urldate = {2020-08-11},
	journal = {Journal of Colloid and Interface Science},
	author = {Huh, Chun and Scriven, L. E},
	month = jan,
	year = {1971},
	pages = {85--101},
	file = {ScienceDirect Snapshot:/home/u1996721/Zotero/storage/CX8NT5VX/0021979771901883.html:text/html;ScienceDirect Full Text PDF:/home/u1996721/Zotero/storage/XNQZZKPI/Huh and Scriven - 1971 - Hydrodynamic model of steady movement of a solidl.pdf:application/pdf}
}

@article{shi_molecular_2009,
	title = {Molecular dynamics simulation of the contact angle of liquids on solid surfaces},
	volume = {130},
	issn = {0021-9606},
	url = {https://0-aip-scitation-org.pugwash.lib.warwick.ac.uk/doi/10.1063/1.3055600},
	doi = {10.1063/1.3055600},
	abstract = {In this work, Lennard-Jones liquid and water droplets are simulated adjacent to a solid surface using molecular dynamics. The contact angle is obtained by using direct simulation. The particle-particle particle-mesh method [B. Shi, S. Sinha, and V. K. Dhir, J. Phys. Chem. 124, 204715 (2006)] for long range force correction is used in the simulation. The contact angle is studied as a function of system temperature and the solid/fluid interaction potential. It is shown that the contact angle decreases with increasing system temperature and increases when the potential decreases. At high system temperature (pressure), the contact angle drops to zero. The predictions are compared with data from experiments and a reasonable agreement is found.},
	number = {3},
	urldate = {2020-08-11},
	journal = {The Journal of Chemical Physics},
	author = {Shi, Bo and Dhir, Vijay K.},
	month = jan,
	year = {2009},
	note = {Publisher: American Institute of Physics},
	pages = {034705},
	file = {Full Text PDF:/home/u1996721/Zotero/storage/77MKG25B/Shi and Dhir - 2009 - Molecular dynamics simulation of the contact angle.pdf:application/pdf;Snapshot:/home/u1996721/Zotero/storage/CEL2TCVE/1.html:text/html}
}

@article{fernandez-toledano_molecular-dynamics_2019,
	title = {A molecular-dynamics study of sliding liquid nanodrops: {Dynamic} contact angles and the pearling transition},
	volume = {548},
	issn = {0021-9797},
	shorttitle = {A molecular-dynamics study of sliding liquid nanodrops},
	url = {http://www.sciencedirect.com/science/article/pii/S0021979719303984},
	doi = {10.1016/j.jcis.2019.03.094},
	abstract = {Hypothesis
That the behavior of sliding drops at the nanoscale mirrors that seen in macroscopic experiments, that the local microscopic contact angle is velocity dependent in a way that is consistent with the molecular-kinetic theory (MKT), and that observations at this scale shed light on the pearling transition seen with larger drops.
Methods
We use large-scale molecular dynamics (MD) to model a nanodrop of liquid sliding across a solid surface under the influence of an external force. The simulations enable us to extract the shape of the drop, details of flow within the drop and the local dynamic contact angle at all points around its periphery.
Findings
Our results confirm the macroscopic observation that the dynamic contact angle at all points around the drop is a function of the velocity of the contact line normal to itself, Ucmsinϕ, where Ucm is the velocity of the drop’s center of mass and ϕ is the slope of the contact line with respect to the direction of travel. Flow within the drop agrees with that observed on the surface of macroscopic drops. If slip between the first layer of liquid molecules and the solid surface is accounted for, the velocity-dependence of the dynamic contact angle is identical with that found previous MD simulations of spreading drops, and consistent with the MKT. If the external force is increased beyond a certain point, the drop elongates and a neck appears between the front and rear of the drop, which separate into two distinct zones. This appears to be the onset of the pearling transition at the tip of a macroscopic drop. The receding contact angle at the tip of the drop is far removed from its equilibrium value but non-zero and approaches a more-or-less constant critical value as the transition progresses.},
	language = {en},
	urldate = {2020-08-12},
	journal = {Journal of Colloid and Interface Science},
	author = {Fernández-Toledano, J. -C. and Blake, T. D. and Limat, L. and De Coninck, J.},
	month = jul,
	year = {2019},
	keywords = {Avoided critical behavior, Microscopic contact angle, Molecular-kinetic theory (MKT), Moving contact lines, Slip, Wetting},
	pages = {66--76},
	file = {ScienceDirect Snapshot:/home/u1996721/Zotero/storage/25VCUDXI/S0021979719303984.html:text/html;ScienceDirect Full Text PDF:/home/u1996721/Zotero/storage/9KDF2WQD/Fernández-Toledano et al. - 2019 - A molecular-dynamics study of sliding liquid nanod.pdf:application/pdf}
}

@book{kampen_stochastic_2007,
	address = {Amsterdam, NETHERLANDS, THE},
	title = {Stochastic {Processes} in {Physics} and {Chemistry}},
	isbn = {978-0-08-047536-3},
	url = {http://ebookcentral.proquest.com/lib/warw/detail.action?docID=291692},
	abstract = {The third edition of Van Kampen's standard work has been revised and updated. The main difference with the second edition is that the contrived application of the quantum master equation in section 6 of chapter XVII has been replaced with a satisfactory treatment of quantum fluctuations. Apart from that throughout the text corrections have been made and a number of references to later developments have been included. From the recent textbooks the following are the most relevant. C.W.Gardiner, Quantum Optics (Springer, Berlin 1991) D.T. Gillespie, Markov Processes (Academic Press, San Diego 1992) W.T. Coffey, Yu.P.Kalmykov, and J.T.Waldron, The Langevin Equation (2nd edition, World Scientific, 2004) Comprehensive coverage of fluctuations and stochastic methods for describing them A must for students and researchers in applied mathematics, physics and physical chemistry},
	urldate = {2020-08-13},
	publisher = {Elsevier Science \& Technology},
	author = {Kampen, N. G. van and Van Kampen, N G},
	year = {2007},
	keywords = {Chemistry, Physical and theoretical - Statistical methods},
	file = {ProQuest Ebook Snapshot:/home/u1996721/Zotero/storage/REH3JQGJ/detail.html:text/html}
}

@techreport{kermode_james_px914_2020,
	title = {{PX914} {Lecture} 4 {Generalised} {Linear} {Models} - from {Least} {Squares} to {Bayesian} {Regression}},
	url = {https://moodle.warwick.ac.uk/pluginfile.php/1490008/mod_resource/content/1/L04-LinearRegression.html},
	author = {Kermode James},
	month = jul,
	year = {2020}
}

@article{young_iii_1805,
	title = {{III}. {An} essay on the cohesion of fluids},
	volume = {95},
	url = {https://royalsocietypublishing.org/doi/10.1098/rstl.1805.0005},
	doi = {10.1098/rstl.1805.0005},
	abstract = {It has already been asserted, by Mr. Monge and others, that the phenomena of capillary tubes are referable to the cohesive attraction of the superficial particles only of the fluids employed, and that the surfaces must consequently be formed into curves of the nature of lintearias, which are supposed to be the results of a uniform tension of a surface, resisting the pressure of a fluid, either uniform, or varying according to a given law. Segner, who appears to have been the first that maintained a similar opinion, has shown in what manner the principle may be deduced from the doctrine of attraction, but his demonstration is complicated, and not perfectly satisfactory; and in applying the law to the forms of drops, he has neglected to consider the very material effects of the double curvature, which is evidently the cause of the want of a perfect coincidence of some of his experiments with his theory. Since the time of Segner, little has been done in investigating accurately and in detail the various consequences of the principle. It will perhaps be most agreeable to the experimental philosopher, although less consistent with the strict course of logical argument, to proceed in the first place to the comparison of this theory with the phenomena, and to inquire afterwards for its foundation in the ultimate properties of matter. But it is necessary to premise one observation, which appears to be new, and which is equally consistent with theory and with experiment; that is, that for each combination of a solid and a fluid, there is an appropriate angle of contact between the surfaces of the fluid, exposed to the air, and to the solid. This angle, for glass and water, and in all cases where a solid is perfectly wetted by a fluid, is evanescent: for glass and mercury, it is about 140°, in common temperatures, and when the mercury is moderately clean.},
	urldate = {2020-08-16},
	journal = {Philosophical Transactions of the Royal Society of London},
	author = {Young, Thomas},
	month = jan,
	year = {1805},
	note = {Publisher: Royal Society},
	pages = {65--87},
	file = {Full Text PDF:/home/u1996721/Zotero/storage/LETPSZJY/Young - 1805 - III. An essay on the cohesion of fluids.pdf:application/pdf;Snapshot:/home/u1996721/Zotero/storage/23WVX8WW/rstl.1805.html:text/html}
}

@article{td_blake_ydshikhmurzaev_dynamic_2002,
	title = {Dynamic {Wetting} by {Liquids} of {Different} {Viscosity}},
	volume = {253},
	issn = {0021-9797},
	url = {https://www.sciencedirect.com/science/article/pii/S0021979702985139},
	doi = {10.1006/jcis.2002.8513},
	abstract = {The velocity-dependence of the dynamic contact angle is studied experimentally for a series of water-glycerol solutions having viscosities ranging fro…},
	language = {en},
	number = {1},
	urldate = {2020-08-16},
	journal = {Journal of Colloid and Interface Science},
	author = {{T.D. Blake, Y.D.Shikhmurzaev}},
	month = sep,
	year = {2002},
	note = {Publisher: Academic Press},
	pages = {196--202},
	file = {Snapshot:/home/u1996721/Zotero/storage/VUFK39SC/S0021979702985139.html:text/html}
}

@article{li_wetting_1994,
	title = {Wetting of ceramic materials by liquid silicon, aluminium and metallic melts containing titanium and other reactive elements: {A} review},
	volume = {20},
	issn = {0272-8842},
	shorttitle = {Wetting of ceramic materials by liquid silicon, aluminium and metallic melts containing titanium and other reactive elements},
	url = {http://www.sciencedirect.com/science/article/pii/0272884294900272},
	doi = {10.1016/0272-8842(94)90027-2},
	abstract = {The wetting properties of ceramic materials by liquid silicon, aluminium and metallic melts containing titanium and other reactive elements are reviewed on the basis of the current understanding and recent developments in the field of metal-ceramic wetting. For silicon and aluminium, attention is paid to the surface characteristics of both metals and ceramics, and to the effect of chemical reactions at the interfaces on the wettability. A special effort is made to analyse the Ti-induced wetting of ceramics in terms of the chemical reactivity and interface microchemistry. The importance of interactions between the interfacially active element (Ti) and other alloying elements in the metallic melts is elucidated with numerous experimental results.},
	language = {en},
	number = {6},
	urldate = {2020-08-16},
	journal = {Ceramics International},
	author = {Li, Jian-Guo},
	month = jan,
	year = {1994},
	pages = {391--412},
	file = {ScienceDirect Snapshot:/home/u1996721/Zotero/storage/523CK9VU/0272884294900272.html:text/html;ScienceDirect Full Text PDF:/home/u1996721/Zotero/storage/VLVHGF44/Li - 1994 - Wetting of ceramic materials by liquid silicon, al.pdf:application/pdf}
}

@article{shikhmurzaev_moving_1997,
	title = {Moving contact lines in liquid/liquid/solid systems},
	volume = {334},
	issn = {1469-7645, 0022-1120},
	url = {https://www.cambridge.org/core/journals/journal-of-fluid-mechanics/article/moving-contact-lines-in-liquidliquidsolid-systems/B4D023934EA4FB3F3FAD4CAE2CB1D4F1},
	doi = {10.1017/S0022112096004569},
	abstract = {A general mathematical model which describes the motion of an
interface between immiscible viscous fluids along a smooth homogeneous
solid
surface is examined in the case of small capillary and Reynolds numbers.
The
model stems from a conclusion that the Young equation,
σ1 cos θ = σ2 − σ3,
which expresses the balance of tangential projection of the forces acting
on the
three-phase contact line in terms of the surface tensions
σi and the contact angle θ, together with
the
well-established experimental
fact that the dynamic contact angle deviates from the static one, imply
that
the surface tensions of contacting interfaces in the immediate vicinity
of the
contact line deviate
from their equilibrium values when the contact line is moving. The same
conclusion
also follows from the experimentally observed kinematics of the flow, which
indicates that liquid particles belonging to interfaces traverse the three-phase
interaction zone
(i.e. the ‘contact line’) in a finite time and become elements
of
another interface – hence their surface properties have to relax
to new
equilibrium values giving rise to
the surface tension gradients in the neighbourhood of the moving contact
line. The
kinematic picture of the flow also suggests that the contact-line motion
is only a
particular case of a more general phenomenon – the process of interface
formation or disappearance – and the corresponding mathematical model
should
be derived from first principles for this general process and then applied
to
wetting as well as to other relevant flows. In the present paper, the simplest
theory which uses this approach is formulated and applied to the moving
contact-line problem. The model describes the true kinematics of the flow
so that
it allows for the ‘splitting’ of the
free surface at the contact line, the appearance of the surface tension
gradients
near the contact line and their influence upon the contact angle and the
flow field. An analytical expression for the dependence of the dynamic
contact
angle on the contact-line speed and parameters characterizing properties
of
contacting media is derived and examined. The role of a ‘thin’
microscopic residual film formed by adsorbed
molecules of the receding fluid is considered. The flow field in the vicinity
of the contact line is analysed. The results are compared with experimental
data obtained for different fluid/liquid/solid systems.},
	language = {en},
	urldate = {2020-08-16},
	journal = {Journal of Fluid Mechanics},
	author = {Shikhmurzaev, Yulii D.},
	month = mar,
	year = {1997},
	note = {Publisher: Cambridge University Press},
	pages = {211--249},
	file = {Full Text PDF:/home/u1996721/Zotero/storage/DC8DF55Q/Shikhmurzaev - 1997 - Moving contact lines in liquidliquidsolid system.pdf:application/pdf;Snapshot:/home/u1996721/Zotero/storage/BETS2VL2/B4D023934EA4FB3F3FAD4CAE2CB1D4F1.html:text/html}
}

@article{hess_determining_2001,
	title = {Determining the shear viscosity of model liquids from molecular dynamics simulations},
	volume = {116},
	issn = {0021-9606},
	url = {https://aip.scitation.org/doi/abs/10.1063/1.1421362},
	doi = {10.1063/1.1421362},
	number = {1},
	urldate = {2020-08-17},
	journal = {The Journal of Chemical Physics},
	author = {Hess, Berk},
	month = dec,
	year = {2001},
	note = {Publisher: American Institute of Physics},
	pages = {209--217},
	file = {Full Text PDF:/home/u1996721/Zotero/storage/GKQQYG2T/Hess - 2001 - Determining the shear viscosity of model liquids f.pdf:application/pdf;Snapshot:/home/u1996721/Zotero/storage/LJ86ZR5I/1.html:text/html}
}

@article{easteal_self-diffusion_1983,
	title = {Self-diffusion in a dense hard-sphere fluid: {A} molecular dynamics simulation},
	volume = {121},
	issn = {0378-4371},
	shorttitle = {Self-diffusion in a dense hard-sphere fluid},
	url = {http://www.sciencedirect.com/science/article/pii/037843718390256X},
	doi = {10.1016/0378-4371(83)90256-X},
	abstract = {Molecular dynamics calculations of the ratio D/DE (where D is the self-diffusion coefficient and DE is the Enskog dense fluid diffusion coefficient) for a dense hard-sphere fluid, have been done for the density range corresponding to 1.5 ⩽ V/V0 ⩽ 4.0 (where V0 is the volume of close-packed hard spheres), for systems of 128, 250 and 432 particles. Values of D/DE at a given density do not differ significantly for 250 and 432 particles, and the values are significantly smaller than those obtained for the same densities by Alder, Gass and Wainwright via application of a hydrodynamic correction to give values for an infinite number of particles. The D/DE values for 250 or 432 particles lead to a much better correlation between the Chandler hard-spheres theory and experimental diffusion data for methane than was obtained previously using the infinite system values of D/DE.},
	language = {en},
	number = {1},
	urldate = {2020-08-17},
	journal = {Physica A: Statistical Mechanics and its Applications},
	author = {Easteal, A. J. and Woolf, L. A. and Jolly, D. L.},
	month = aug,
	year = {1983},
	pages = {286--292},
	file = {ScienceDirect Snapshot:/home/u1996721/Zotero/storage/KFMFR4QA/authorization.html:text/html;ScienceDirect Full Text PDF:/home/u1996721/Zotero/storage/JKKKTJ6P/Easteal et al. - 1983 - Self-diffusion in a dense hard-sphere fluid A mol.pdf:application/pdf}
}

@article{terence_d_blake_physics_2006,
	title = {The physics of moving wetting lines},
	volume = {299},
	issn = {0021-9797},
	url = {https://www.sciencedirect.com/science/article/pii/S0021979706002463},
	doi = {10.1016/j.jcis.2006.03.051},
	abstract = {Scientists tend to think in terms of their most familiar models. It is not accidental that the earliest descriptions of the moving wetting line and it…},
	language = {en},
	number = {1},
	urldate = {2020-08-17},
	journal = {Journal of Colloid and Interface Science},
	author = {{Terence D. Blake}},
	month = jul,
	year = {2006},
	note = {Publisher: Academic Press},
	pages = {1--13},
	file = {Snapshot:/home/u1996721/Zotero/storage/IC8WTUAB/S0021979706002463.html:text/html}
}

@article{chen_convex_2014,
	title = {Convex {Nanobending} at a {Moving} {Contact} {Line}: {The} {Missing} {Mesoscopic} {Link} in {Dynamic} {Wetting}},
	volume = {8},
	issn = {1936-0851},
	shorttitle = {Convex {Nanobending} at a {Moving} {Contact} {Line}},
	url = {https://doi.org/10.1021/nn5046486},
	doi = {10.1021/nn5046486},
	abstract = {The morphological information on the very front of a spreading liquid is fundamental to our understanding of dynamic wetting. Debate has lasted for years concerning the nanoscopic local angles and the transition from them to the macroscopic counterpart, θD. This study of nonvolatile liquids analyzes the interface profile near the advancing contact line using an advanced atomic force microscopy. The interface is found following the macroscopic profile until bending in a convex profile around 20 nm from the substrate. This shoe-tip-like feature is common in partially wetting while absent for completely wetting, and its curvature varies with advancing speed. The observation ends the long-standing debate about the nanoscopic contact angles and their speed dependency. The convex nanobending provides a mesoscopic link and effectively complicates the dynamic wetting behaviors.},
	number = {11},
	urldate = {2020-08-20},
	journal = {ACS Nano},
	author = {Chen, Lei and Yu, Jiapeng and Wang, Hao},
	month = nov,
	year = {2014},
	note = {Publisher: American Chemical Society},
	pages = {11493--11498},
	file = {Full Text PDF:/home/u1996721/Zotero/storage/VNEXUC4C/Chen et al. - 2014 - Convex Nanobending at a Moving Contact Line The M.pdf:application/pdf;ACS Full Text Snapshot:/home/u1996721/Zotero/storage/5EQWS3F7/nn5046486.html:text/html}
}

@article{bertrand_dynamics_2007,
	title = {Dynamics of {Dewetting} at the {Nanoscale} {Using} {Molecular} {Dynamics}},
	volume = {23},
	issn = {0743-7463},
	url = {https://doi.org/10.1021/la062920m},
	doi = {10.1021/la062920m},
	abstract = {Large-scale molecular dynamics simulations are used to model the dewetting of solid surfaces by partially wetting thin liquid films. Two levels of solid−liquid interaction are considered that give rise to large equilibrium contact angles. The initial length and thickness of the films are varied over a wide range at the nanoscale. Spontaneous dewetting is initiated by removing a band of molecules either from each end of the film or from its center. As observed experimentally and in previous simulations, the films recede at an initially constant speed, creating a growing rim of liquid with a constant receding dynamic contact angle. Consistent with the current understanding of wetting dynamics, film recession is faster on the more poorly wetted surface to an extent that cannot be explained solely by the increase in the surface tension driving force. In addition, the rates of recession of the thinnest films are found to increase with decreasing film thickness. These new results imply not only that the mobility of the liquid molecules adjacent to the solid increases with decreasing solid−liquid interactions, but also that the mobility adjacent to the free surface of the film is higher than in the bulk, so that the effective viscosity of the film decreases with thickness.},
	number = {7},
	urldate = {2020-08-20},
	journal = {Langmuir},
	author = {Bertrand, E. and Blake, T. D. and Ledauphin, V. and Ogonowski, G. and De Coninck, J. and Fornasiero, D. and Ralston, J.},
	month = mar,
	year = {2007},
	note = {Publisher: American Chemical Society},
	pages = {3774--3785},
	file = {Full Text PDF:/home/u1996721/Zotero/storage/HIB37DFQ/Bertrand et al. - 2007 - Dynamics of Dewetting at the Nanoscale Using Molec.pdf:application/pdf;ACS Full Text Snapshot:/home/u1996721/Zotero/storage/MEPJYV8E/la062920m.html:text/html}
}

@article{bertrand_influence_2009,
	title = {Influence of solid–liquid interactions on dynamic wetting: a molecular dynamics study},
	volume = {21},
	issn = {0953-8984},
	shorttitle = {Influence of solid–liquid interactions on dynamic wetting},
	url = {https://doi.org/10.1088%2F0953-8984%2F21%2F46%2F464124},
	doi = {10.1088/0953-8984/21/46/464124},
	abstract = {Large-scale molecular dynamics (MD) simulations of liquid drops spreading on a solid substrate have been carried out for a very wide range of solid–liquid interactions and equilibrium contact angles. The results for these systems are shown to be consistent with the molecular-kinetic theory (MKT) of dynamic wetting, which emphasizes the role of contact-line friction as the principal channel of energy dissipation. Several predictions have been confirmed. These include a quantitative link between the dynamics of wetting and the work of adhesion and the existence of an optimum equilibrium contact angle that maximizes the speed of wetting. A feature of the new work is that key parameters (κ0 and λ), normally accessible only by fitting the MKT to dynamic contact angle data, are also obtained directly from the simulations, with good agreement between the two sources. This validates the MKT at some fundamental level. Further verification is provided by contact angle relaxation studies, which also lend support to the interfacial tension relaxation process invoked in Shikhmurzaev’s hydrodynamic model of dynamic wetting.},
	language = {en},
	number = {46},
	urldate = {2020-08-20},
	journal = {Journal of Physics: Condensed Matter},
	author = {Bertrand, Emilie and Blake, Terence D. and Coninck, Joël De},
	month = oct,
	year = {2009},
	note = {Publisher: IOP Publishing},
	pages = {464124},
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@book{acheson_elementary_1990,
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repository: JingBang-Liu/MovingContactLine

repo_name: JingBang-Liu/MovingContactLine


text:
@incollection{liu2018data,
 author = {Liu, Zeliang and Kafka, Orion L and Yu, Cheng and Liu, Wing Kam},
 booktitle = {Advances in computational plasticity},
 pages = {221--242},
 publisher = {Springer},
 title = {Data-driven self-consistent clustering analysis of heterogeneous materials with crystal plasticity},
 year = {2018}
}


text:
@article{annavajhala2021emergence,
  title={Emergence and expansion of SARS-CoV-2 B. 1.526 after identification in New York},
  author={Annavajhala, Medini K and Mohri, Hiroshi and Wang, Pengfei and Nair, Manoj and Zucker, Jason E and Sheng, Zizhang and Gomez-Simmonds, Angela and Kelley, Anne L and Tagliavia, Maya and Huang, Yaoxing and others},
  journal={Nature},
  volume={597},
  number={7878},
  pages={703--708},
  year={2021},
  publisher={Nature Publishing Group}
}