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Equilibrium dynamics using XPCS Block copolymers present an interesting class of materials with a broad range of applications. The fact that these molecules self-assemble on length scales ~10nm makes them ideally suited to various nanotechnology applications including memory devices, photonic bandgap materials and lithium batteries to name a few. In recent years, a lot of work, both experimental as well as theoretical, has been done towards understanding the thermodynamic properties of block copolymers and extensive phase diagrams have been mapped for several systems. However, the understanding of the dynamics of these materials on a microscopic length scale is still in its infancy. In this project, we attempt to shed light on structural relaxation dynamics of a poly(styrene-block-isoprene) block copolymer using the conventional rheological techniques as well as a recently developed technique: X-ray Photon Correlation Spectroscopy (XPCS). We start by characterizing the equilibrium thermodyamic structure at various temperatures. Below the order-to-disorder transition temperature (TODT) of 70C, the polymer exists in the form of hexagonally packed cylinders. Above TODT there is an equilibrium volume fraction of disordered micelles dispersed in a homogenous matrix.(1) As the temperature is increased further, the volume fraction of the micelles decreases and at ~120C, we see no signatures of the presence of the micelles. We begin the dynamic studies in the region above TODT. Macroscopic rheological measurements in this region exhibit terminal behavior, allowing us to obtain a terminal stress relaxation time, tau_tr, commonly known as the longest relaxation time. On the other hand, XPCS measures the dynamic structure factor, which gives us the time it takes for microscopic concentration fluctuations to relax, tau_fluc.
We observe that tau_fluc is 1-2 orders of magnitude larger than the so-called longest relaxation time, tau_tr (Fig. 1). Even though our system contains micelles in a homogenous disordered bulk, we compare it with a theory for a purely disordered system that was proposed by Fredrickson and Larson.(2) The theory captures the effect of simple (non-micellar) concentration fluctuations on tau_fluc and is called tau_FL (Fig. 1). There is qualitative agreement between theory and experiment in that tau_fluc>tau_tr. However, a lack of quantitative agreement suggests that the origin of the tau_fluc is linked to the presence of the micelles. The relaxation of a micellar phase can, in principle, be a result of either the dissolution of micelles or the diffusion of intact micelles. On comparing tau_fluc to the Stokes-Einstein diffusion time, tau_diff, we find good quantitative agreement. This suggests that the relaxation mode measured by XPCS is that of micelle diffusion and that micelle dissolution does not occur on the time scale given by tau_fluc.
1. "Structure and phase behavior of block copolymer melts near
the sphere-cylinder boundary", F. M. Abuzaina, A. J. Patel, S.
Mochrie, S. Narayanan, A. Sandy, B. A. Garetz and N. P. Balsara, vol.
38, p. 7090-7097, Macromolecules, 2005. |
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