Agra-Kooijman Dena M, Fisch Michael R, Joshi Leela, Ren Wanting, McMullan Philip J, Griffin Anselm C, Kumar Satyendra
Department of Physics, Kent State University, Kent, OH 44242, USA.
Phys Chem Chem Phys. 2015 Jan 7;17(1):191-9. doi: 10.1039/c4cp04713c.
The relationship between strain-dependent macroscopic elastic behavior and the changes in microscopic structure of the smectic-C liquid crystal elastomer (LCE), C11MeHQSi8 were investigated using synchrotron X-ray studies. At very low strains ε ≤ 0.2, the smectic layers are randomly oriented. As the strain increases beyond 0.2, the smectic layers reorient and become parallel to the direction of the applied strain. The polydomain to monodomain (P-M) transition accompanied by the formation of chevron structure ensues for ε > 0.2 and is nearly complete for ε = 0.7. The chevron structure relaxes after the applied strain changes, with a time constant τα ∼ 45 min while the orientation order parameters of the mesogenic and elastomeric components gradually increase and saturate at 0.83 and 0.4, respectively at ε = 1.7 which is near the end of the plateau region. Relaxation rates τα for the tilt angle and τd corresponding to the smectic layer spacing both become about 10 times faster when the strain exceeds 0.7. The LCE remains "locked" into the monodomain state and retains 90% and 80% values of α and S, respectively for 24 hours after the applied strain is removed. The viscoelastic properties of the liquid crystal appear to dominate the equilibration process at low strains while the elastomeric properties control the system's response at high strains.
利用同步加速器X射线研究,对近晶C型液晶弹性体(LCE)C11MeHQSi8的应变依赖宏观弹性行为与微观结构变化之间的关系进行了研究。在非常低的应变ε≤0.2时,近晶层随机取向。当应变增加超过0.2时,近晶层重新取向并变得与施加应变的方向平行。对于ε>0.2,伴随着人字形结构的形成会发生多畴到单畴(P-M)转变,而对于ε = 0.7时转变几乎完成。在施加的应变改变后,人字形结构会松弛,时间常数τα约为45分钟,而介晶和弹性体组分的取向序参数在ε = 1.7(接近平台区末端)时分别逐渐增加并饱和到0.83和0.4。当应变超过0.7时,倾斜角的松弛速率τα和对应于近晶层间距的τd都加快约10倍。在去除施加的应变后,LCE保持“锁定”在单畴状态,并分别在24小时内保留α和S值的90%和80%。在低应变下,液晶的粘弹性性质似乎主导了平衡过程,而在高应变下弹性体性质控制了系统的响应。