Scaling Model of Low-Temperature Transport Properties for Molecular and Ionic Liquids

<div>Comparison of heat conductivities predicted (curves) by universal (argon-based) scaling function (<a href="https://static.hindawi.com/articles/jther/volume-2015/208486/figures/#EEq22">20</a>) with experimental data (points) at <svg height="11.7574pt" id="M228" style="vertical-align:-3.16066pt" version="1.1" viewbox="-0.0498162 -8.59674 45.123 11.7574" width="45.123pt" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink"><g transform="matrix(.013,0,0,-0.013,0,0)"><path d="M622 479C622 589 545 650 400 650H146L140 618C229 609 230 602 215 527L135 132C117 43 112 41 27 32L18 0H305L313 32C213 40 205 44 222 132L251 284L324 262H365C484 269 622 333 622 479ZM528 477C528 356 420 305 344 305C300 305 276 314 259 321L303 554C311 597 313 600 331 606C345 611 361 614 379 614C463 614 528 580 528 477Z" id="g50-81"></path><glyph.data ascent="3443" descent="-2856" horiz-adv-x="640" vert-adv-y="640"></glyph.data></g><g transform="matrix(.0091,0,0,-0.0091,6.721,3.001)"><path d="M245 635C92 635 37 457 37 312C37 149 91 -12 244 -12C395 -12 449 166 449 312C449 469 395 635 245 635ZM243 598C332 598 358 454 358 312C358 173 334 26 245 26C158 26 128 174 128 313S152 598 243 598Z" id="g50-49"></path><glyph.data ascent="3443" descent="-2856" horiz-adv-x="487" vert-adv-y="487"></glyph.data></g><g transform="matrix(.013,0,0,-0.013,15.343,0)"><path d="M556 363L527 402C504 370 473 342 434 342C405 342 359 363 323 381C278 403 224 427 181 427C130 427 88 391 55 350L88 314C111 346 142 374 181 374C210 374 256 353 292 335C337 312 383 289 434 289C484 289 525 323 556 363ZM556 172L527 211C504 179 473 151 434 151C405 151 359 172 323 190C278 212 224 236 181 236C130 236 88 200 55 159L88 123C111 155 142 183 181 183C210 183 256 162 292 144C337 121 383 98 434 98C484 98 525 132 556 172Z" id="g54-132"></path><glyph.data ascent="3443" descent="-2856" horiz-adv-x="611" vert-adv-y="611"></glyph.data></g><g transform="matrix(.013,0,0,-0.013,26.961,0)"><path d="M245 635C92 635 37 457 37 312C37 149 91 -12 244 -12C395 -12 449 166 449 312C449 469 395 635 245 635ZM243 598C332 598 358 454 358 312C358 173 334 26 245 26C158 26 128 174 128 313S152 598 243 598Z" id="g50-49"></path><glyph.data ascent="3443" descent="-2856" horiz-adv-x="487" vert-adv-y="487"></glyph.data></g><g transform="matrix(.013,0,0,-0.013,33.292,0)"><path d="M98 134C72 134 46 117 46 90C46 73 55 65 60 64C95 55 124 32 124 -4C124 -42 95 -68 44 -89L57 -123C122 -104 194 -60 194 22C194 94 136 134 98 134Z" id="g50-45"></path><glyph.data ascent="3443" descent="-2856" horiz-adv-x="237" vert-adv-y="237"></glyph.data></g><g transform="matrix(.013,0,0,-0.013,38.578,0)"><path d="M389 0V32C297 38 291 46 291 118V635C234 613 175 595 109 583V556L161 554C203 552 207 547 207 497V118C207 46 201 38 110 32V0H389Z" id="g50-50"></path><glyph.data ascent="3443" descent="-2856" horiz-adv-x="487" vert-adv-y="487"></glyph.data></g></svg> MPa.</div>

Journal of Thermodynamics

fig3

Figure 3

Figure 3: Scaling Model of Low-Temperature Transport Properties for Molecular and Ionic Liquids 