Kulkarni, SiddharthSiddharthKulkarniThareja, PrachiPrachiThareja2025-08-302025-08-302017-10-0110.1007/s00397-017-1039-72-s2.0-85029010522https://d8.irins.org/handle/IITG2025/22376We study the influence of confinement on the rheology and structure of nematic liquid crystals (NLCs). NLCs get confined in networks of titania (TiO<inf>2</inf>, primary particle size = 21 nm) nanoparticles in suspensions of TiO<inf>2</inf> and NLC, N-(4-methoxybenzylidene)-4-butylaniline (MBBA). Suspensions with TiO<inf>2</inf> nanoparticle volume fraction (ϕ) of 0.006–0.017, form viscoelastic solids with low elastic modulus (G′) of 10¹ Pa–10² Pa and short relaxation times. Increase in TiO<inf>2</inf> nanoparticle ϕ leads to a rise in G′ with TiO<inf>2</inf> nanoparticles forming a percolating network at a critical volume fraction (ϕ<inf>c</inf>) = 0.023, and G′ of ~10³ Pa. TiO<inf>2</inf>/MBBA NLC suspensions at and above ϕ<inf>c</inf> = 0.023 show G′ ~ ω^x−1 scaling, where ω is the angular frequency and the minimum in loss modulus (G′′) with ω. The effective noise temperature, x decreases and approaches 1 with the increase in the TiO<inf>2</inf> nanoparticle ϕ from 0.023–0.035, is indicative of an increase in the glassy dynamics. Through the polarized light microscopy and differential scanning calorimetry experiments, we propose that the progressive addition of TiO<inf>2</inf> nanoparticles introduces a quenched random disorder (QRD) in the NLC medium which disturbs the nematic order. This results in metastable TiO<inf>2</inf>/MBBA NLC suspensions in which NLC domains get confined in the network of flocs of TiO<inf>2</inf> nanoparticles. We also show that the salient rheological signatures of soft glassy rheology develop only in the presence of NLC MBBA and are absent in the isotropic phase of MBBA.falseNematic liquid crystals | Quenched random disorder | Soft glassy rheologyArticle825-8401 October 20172arJournal2WOS:000410747200005