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首页> 外文期刊>Physical chemistry chemical physics: PCCP >Micelles and gels of oxyethylene-oxybutylene diblock copolymers in aqueous solution: The effect of oxyethylene-block length
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Micelles and gels of oxyethylene-oxybutylene diblock copolymers in aqueous solution: The effect of oxyethylene-block length

机译:水溶液中氧乙烯-氧丁烯二嵌段共聚物的胶束和凝胶:氧乙烯嵌段长度的影响

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摘要

Block copolymer E_(90)B_(10) (E = oxyethylene, B = oxybutylene) was synthesised and characterised by gel permeation chromatography and ~(13)C NMR spectroscopy. Dynamic light scattering (DLS) and static light scattering (SLS) were used to characterise the micelles in solution (both in water and in aqueous 0.2 mol dm~(-1) K_2SO_4), yielding the micellar association numbers, the hydrodynamic and thermodynamic radii, and related expansion factors. Micellar parameters were also obtained by small-angle neutron scattering (SANS) for solutions of a similar copolymer, E_(86)B_(10), in water, i.e., the association number, the hard-sphere radius, the micelle volume fraction and the corresponding expansion factors. A comparison of the appropriate quantities showed good agreement between the two techniques. SANS gave additional information e.g., volume fraction profiles for the micelles and volume fraction of water in the micelle core. Moderately concentrated solutions of copolymer E_(90)B_(10) were studied in the gel state by small-angle X-ray scattering (SAXS) in tandem with rheology (oscillatory shear). Values for the dynamic elastic modulus (G') of the gels significantly exceeded 10~4 Pa across the range of temperature (25-80 deg C) and frequency (0.1-100 rad s~(-1)) explored. The SAXS patterns for the orientated gels showed them to have a body-centred-cubic structure, as expected for packed, spherical micelles. This structure persisted over a wide concentration range, e.g., until crystallisation of the E blocks occurred at high concentration (>= 70 wt.% copolymer). By combining the present and published results, a comparison was made of the micelle and gel properties of copolymers with the same B-block length but different E-block lengths, i.e., E_(90)B_(10), E_(40)B_(10) and E_(18)B_(10). As would be expected, as the E-block length was increased, the micelle association numbers decreased while the micelle radii and expansion factors increased. The critical gel concentration (cgc) also decreased as the E-block length was increased. Moreover, the cgc correlated quantitatively with the thermodynamic expansion factors obtained by SLS and SANS from the exclusion properties of the micelles.
机译:合成了嵌段共聚物E_(90)B_(10)(E =氧乙烯,B =氧丁烯),并通过凝胶渗透色谱和〜(13)C NMR光谱进行了表征。用动态光散射(DLS)和静态光散射(SLS)表征溶液中的​​胶束(在水中和在0.2 mol dm〜(-1)K_2SO_4水溶液中),得到胶束缔合数,流体力学和热力学半径,以及相关的扩展因子。还通过小角度中子散射(SANS)获得了类似共聚物E_(86)B_(10)在水中的溶液的胶束参数,即缔合数,硬球半径,胶束体积分数和相应的扩展因子。适当数量的比较显示了两种技术之间的良好一致性。 SANS提供了其他信息,例如,胶束的体积分数分布和胶束核心中水的体积分数。通过流变学(振荡剪切),通过小角X射线散射(SAXS)研究了处于凝胶状态的共聚物E_(90)B_(10)的中浓溶液。在探索的温度(25-80摄氏度)和频率(0.1-100 rad s〜(-1))范围内,凝胶的动态弹性模量(G')值明显超过10〜4 Pa。定向凝胶的SAXS模式显示它们具有以身体为中心的立方结构,这对于填充的球形胶束是期望的。该结构在宽的浓度范围内持续存在,例如,直到在高浓度下发生E嵌段的结晶(≥70重量%的共聚物)。通过结合现有和公开的结果,对具有相同B嵌段长度但E嵌段长度不同(即E_(90)B_(10),E_(40)B_)的共聚物的胶束和凝胶性质进行了比较。 (10)和E_(18)B_(10)。如预期的那样,随着E-嵌段长度的增加,胶束缔合数减少,而胶束半径和膨胀因子增加。临界凝胶浓度(cgc)也随着E嵌段长度的增加而降低。此外,cgc与SLS和SANS从胶束的排斥特性获得的热力学膨胀因子定量相关。

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