Electronic Supplementary Material (ESI) for Soft Matter This journal is © The Royal Society of Chemistry 2013 Supplementary Information Colloid-in-Liquid Crystal Gels Formed via Spinodal Decomposition Emre Bukusoglu,*a Santanu Kumar Pal,b Juan J. de Pabloc,d and Nicholas L. Abbott*a a Department of Chemical and Biological Engineering, University of Wisconsin-Madison, 1415 Engineering Drive, Madison, WI, 53706, USA. Fax: +1 608-262-5434; Tel: +1 608-265-5278; E-mail: [email protected] b Department of Chemical Sciences, Indian Institute of Science Education and Research (IISER) Mohali, Sector-81, SAS Nagar, Mohali, 140306, c Institute of Molecular Engineering, University of Chicago, Chicago, IL, 60637, USA. d Argonne National Laboratory, 9700 South Cass Avenue, Building 223, Argonne, IL, 60439, USA. Dynamics of growth of nematic domains during formation of CLC gels Figure SI.1 A and B show the growth of nematic domains in PS-colloid/E7 samples as a function of temperature (SI.1A and 1B). Figure SI.1C compares the growth characteristics of the nematic domains in the PS-colloid/E7 samples to the growth characteristics of the nematic domains in the CLC gels described by Vollmer et al.1 1 Electronic Supplementary Material (ESI) for Soft Matter This journal is © The Royal Society of Chemistry 2013 AB20 14 18 12 m) m) 16 Domain a μ μ ( ( 14 Domain a1 10 Size Size Domain a2 12 8 10 Domain a3 Domain a4 8 6 Domain b Domain Domain Domain a5 Domain b1 LC LC 6 4 Domain a6 Domain b2 4 Domain a7 2 Domain b3 2 Nematic Domain b4 Nematic 0 0 60.0 59.5 59.0 58.5 58.0 57.5 57.0 56.5 60.0 59.5 59.0 58.5 58.0 57.5 Temperature (ᵒC) Temperature (ᵒC) Domain a C Domain Domain Domain a1 growth growth Domain a2 starts stops Domain a3 Study Domain a4 Our Domain a5 Domain a6 Domain a7 Domain b Domain b1 Study Domain b2 Domain b3 Our Domain b4 Domain 1 Domain 2 Domain 3 Domain 4 Domain 5 al. Domain 6 et Domain 7 Domain 8 Domain 9 Domain 10 Vollmer Domain 11 Domain 12 Domain 13 Tni of pure LC Domain 14 Domain 15 0.5 0 ‐0.5 ‐1 ‐1.5 ‐2 ‐2.5 ‐3 ‐3.5 TT‐‐TTni( (C)ᵒC) ni Figure SI.1. Growth characteristics of nematic domains during formation of CLC gels. (A) PS- colloid/E7 mixtures. Size of Domain a of Figure 1 of main text and neighboring domains which are labeled a1 to a7, (B) Size of Domain b of Figure 1 of main text and neighboring domains labeled as b1 to b4 (C) Comparison of growth characteristics of nematic domains observed with PS-colloid/E7 mixtures to the growth characteristics of nematic domains of PMMS/5CB mixtures reported in Figure 2 of Vollmer et al.1 2 Electronic Supplementary Material (ESI) for Soft Matter This journal is © The Royal Society of Chemistry 2013 Figure SI.2. (A) Polarized light (left) and corresponding brightfield (right) images of a 13.3 wt% PS-colloid/E7 mixture at room temperature. (B) Fluorescence (left) and corresponding brightfield images (right) of a 13.3 wt% PS-colloid/E7 mixture doped with 0.1% Nile Red at room temperature. (Scale bars correspond to 30 μm) 3 Electronic Supplementary Material (ESI) for Soft Matter This journal is © The Royal Society of Chemistry 2013 Dynamics of Evolution of Area Fraction of Phases and Domain Size A thin film of 13.3 wt% PS-colloid/E7 gel was heated to 80.0°C, and then cooled at a rate of 0.2°C/min to 63.0°C (same cooling rate as used in Figure 1) at which temperature the system formed a cellular microstructure. Subsequently, images were recorded while holding the sample at a constant temperature of 63.0°C for ~5 hours (Figure SI.3). Figure SI.3. Isothermal time-lapse brightfield images of a mixture of 13.3 wt% PS-colloids and E7. The images were recorded after the sample had been cooled at a rate of 0.2˚C/min to 63˚C (at t=0 h). The plot in the lower panel shows the area fraction of the E7-rich phase and the average size of E7-rich domains. 4 Electronic Supplementary Material (ESI) for Soft Matter This journal is © The Royal Society of Chemistry 2013 Figure SI.4. Duplicate DSC scans of a 13.3 wt % PS-colloid/E7 sample. The sample was cooled at 5.0 °C/min. The temperature at which phase separation of the colloids in isotropic E7 was observed is indicated as TPS. From the DSC scan shown in Figure SI.4, we determined TNI of a 13.3 wt% PS-colloid/E7 sample to be ~59.5°C. This value is in good agreement with the value of TNI determined by optical microscopy (59.4°C). In addition to TNI, we observed a small exothermic process to occur at a temperature that coincided with the onset of the phase separation of the PS-colloids in the isotropic phase of E7. We note that the temperature at which the onset of phase separation of the PS-colloids was observed in E7 was dependent on the thickness of the sample. When using thick samples (thickness greater than 20m), phase separation of the PS-colloids in E7 was determined by microscopy to occur at 76°C (for 13.3 wt% sample). This temperature coincides with the exothermic signature in the DSC thermogram shown in Figure SI.4. 5 Electronic Supplementary Material (ESI) for Soft Matter This journal is © The Royal Society of Chemistry 2013 Images of initial stage of phase separation The brightfield optical micrographs in Figure SI.5 show the initial stages of phase separation of a 13.3 wt% PS-colloid/E7 mixture after the system was quenched to 67.0°C. Figure SI.5. Time-lapse images of a 13.3 wt% sulfate-PS/E7 mixture quenched to 67.0ᵒC from 71.0ᵒC. 6 Electronic Supplementary Material (ESI) for Soft Matter This journal is © The Royal Society of Chemistry 2013 Figure SI.6. Illustration of the procedure used for the FFT analysis of thin films of 13.3 wt% PS- colloids in E7. 7 Electronic Supplementary Material (ESI) for Soft Matter This journal is © The Royal Society of Chemistry 2013 Characterization of the Coarsening of the Microstructure: A thin film of a 13.3 wt% sulfate-PS/E7 mixture was quenched sequentially to 61 °C from 80 °C, and then to 55 °C from 61 °C. The images were analyzed as described in Figure SI.6. We note that the depth of the quench used to prepare the sample in Figure SI.7 was greater than that used to prepare the samples that are described in Figure 8. Past studies have demonstrated that deep quenches can result in high rates of coarsening due to “viscous hydrodynamic” mechanisms.2, 3 For this reason, the coarsening seen in Figure 8 cannot be directly compared to Figure SI.7. 0.6 0.5 y = 0.0013x + 0.508 0.4 R² = 0.0536 55oC quench o 0.3 61 C quench y = ‐0.2982x + 2.9176 ) y = ‐0.4132x + 3.5977 R² = 0.7802 max 0.2 R² = 0.9796 ln(Q 0.1 0 ‐0.1 ‐0.2 024681012 ln(time(s)) Figure SI.7. Time-dependence of the structural peak in a 13.3 wt% sulfate-PS/E7 mixture quenched from 80°C to 61 °C and then to 55 °C. 8 Electronic Supplementary Material (ESI) for Soft Matter This journal is © The Royal Society of Chemistry 2013 SI References 1. D. Vollmer, G. Hinze, B. Ullrich, W. C. K. Poon, M. E. Cates and A. B. Schofield, Langmuir, 2005, 21, 4921‐4930. 2. E. D. Siggia, Physical Review A, 1979, 20, 595‐605. 3. A. J. Bray, Advances in Physics, 2008. 9 .