Investigation of anisotropic thermal conductivity of uniaxial and biaxial Gay-Berne particles with molecular dynamics simulation

Yildirim A., Eroglu E., Yilmaz S.

MOLECULAR SIMULATION, cilt.37, sa.14, ss.1179-1185, 2011 (SCI-Expanded) identifier identifier

  • Yayın Türü: Makale / Tam Makale
  • Cilt numarası: 37 Sayı: 14
  • Basım Tarihi: 2011
  • Doi Numarası: 10.1080/08927022.2011.589051
  • Dergi Adı: MOLECULAR SIMULATION
  • Derginin Tarandığı İndeksler: Science Citation Index Expanded (SCI-EXPANDED), Scopus
  • Sayfa Sayıları: ss.1179-1185
  • Anahtar Kelimeler: liquid crystal molecules, molecular dynamics simulation, Muller-Plathe method, thermal conductivity, NEMATIC LIQUID-CRYSTALS, MONTE-CARLO, COMPUTER-SIMULATION, HEAT-FLOW, MODEL, FLUID, TRANSITION, BULK
  • Akdeniz Üniversitesi Adresli: Hayır

Özet

In this study, we investigated uniaxial and biaxial Gay-Berne (GB) particles with the help of the molecular dynamics (MD) simulation. Anisotropic thermal conductivities of the uniaxial and biaxial GB liquid crystal molecules were calculated both in the random molecular orientation and in the molecular orientations of 0 degrees, 45 degrees and 90 degrees using the Muller-Plathe method. In the uniaxial molecules, it was found that the thermal conductivity ratios between the parallel and perpendicular components for the smectic and nematic phases are about 2.2:1 and 2.8:1, respectively. As for biaxial molecules, these ratios between the parallel and perpendicular components of molecules for the smectic and nematic phases are about 3.9:1 and 3.8:1, respectively.

In this study, we investigated uniaxial and biaxial Gay–Berne (GB) particles with the help of the molecular dynamics (MD) simulation. Anisotropic thermal conductivities of the uniaxial and biaxial GB liquid crystal molecules were calculated both in the random molecular orientation and in the molecular orientations of 0°, 45° and 90° using the Müller-Plathe method. In the uniaxial molecules, it was found that the thermal conductivity ratios between the parallel and perpendicular components for the smectic and nematic phases are about 2.2:1 and 2.8:1, respectively. As for biaxial molecules, these ratios between the parallel and perpendicular components of molecules for the smectic and nematic phases are about 3.9:1 and 3.8:1, respectively