Bravo-Anaya L Mónica, Roux Denis C D, Soltero Martínez J Félix Armando, Carvajal Ramos Francisco, Pignon Frédéric, Mannix Oonagh, Rinaudo Marguerite
University Grenoble Alpes, CNRS, Grenoble INP, LRP, F-38000 Grenoble, France.
Departamento de Ingeniería Química, Universidad de Guadalajara, Blvd. M. García Barragán #1451, Guadalajara C.P. 44430, México.
Polymers (Basel). 2018 Oct 28;10(11):1204. doi: 10.3390/polym10111204.
Previous investigations were conducted on two concentrations of DNA solution: 4 mg/mL, for which it has been shown that no supramolecular organization is induced under flow at low shear rates; and 10 mg/mL, in which a liquid crystalline-type texture is formed under flow at low shear rates, attesting to an orientation of pre-organized chains. Rheological experiments are discussed and their results supported by small-angle X-ray scattering (SAXS) and flow birefringence visualization experiments. Scattering from polyelectrolytes has a characteristic signal, which is here observed in SAXS, showing a strong correlation peak between charged chains in water, for both concentrations. This peak is weaker in the presence of 0.01 M NaCl and suppressed in salt excess at 0.1 M NaCl. No plateau in the ( γ ˙ ) plot was observed in analysis of rheological experiments on low DNA concentration (4 mg/mL). As typically observed in polyelectrolyte systems both the dynamic moduli and shear viscosity were higher in water as electrostatic forces dominate, than in the presence of salt, especially at low shear rates. The rheological results for concentrations of 0.01 M NaCl are lower than in water as expected due to partial screening of electrostatic repulsions. Rheological data for concentrations of 0.1 M NaCl are unexpected. Electrostatic forces are partially screened in the low salt concentration, leading to a drop in the rheological values. For high salt concentration there are no longer interchain repulsions and so steric interactions dominate within the entangled network leading to the subsequent increase in rheological parameters. Regardless of the solvent, at high shear rates the solutions are birefringent. In the 10 mg/mL case, under flow, textures are formed at relatively low shear rate before all the chains align going to a pseudonematic liquid crystalline phase at high shear rate. The electrostatic repulsion between semi-rigid chains induces a correlation between the chains leading to an electrostatic pseudo-gel in water and loosely in 0.01 M NaCl at low stress applied. To the best of our knowledge, this is the first time that such behavior is observed. In 0.1 M NaCl, DNA behavior resembles the corresponding neutral polymer as expected for polyelectrolyte in salt excess, exhibiting a yield stress. When texture appears in water and in 0.01 M NaCl, a critical transition is observed in rheological curves, where the viscosity decreases sharply at a given critical shear stress corresponding to a plateau in the ( γ ˙ ) plot also observed in creep transient experiment.
先前的研究针对两种浓度的DNA溶液展开:4 mg/mL,已表明在低剪切速率的流动条件下不会诱导超分子结构的形成;以及10 mg/mL,在低剪切速率的流动条件下会形成液晶型织构,证明预组织化链的取向。文中讨论了流变学实验,并通过小角X射线散射(SAXS)和流动双折射可视化实验支持了实验结果。聚电解质的散射具有特征信号,在SAXS中观察到,对于两种浓度,均显示出水中带电链之间有很强的相关峰。在0.01 M NaCl存在时,该峰较弱,而在0.1 M NaCl的盐过量情况下则被抑制。在低DNA浓度(4 mg/mL)的流变学实验分析中,未观察到(γ˙)图中的平台期。正如在聚电解质体系中通常观察到的那样,由于静电力起主导作用,与存在盐的情况相比,尤其是在低剪切速率下,水中的动态模量和剪切粘度更高。0.01 M NaCl浓度下的流变学结果低于水中的结果,这是由于静电排斥力部分被屏蔽所致。0.1 M NaCl浓度下的流变学数据出乎意料。在低盐浓度下静电作用力部分被屏蔽,导致流变学值下降。对于高盐浓度,链间不再有排斥力,因此在缠结网络中空间相互作用占主导,导致流变学参数随后增加。无论溶剂如何,在高剪切速率下溶液都是双折射的。在10 mg/mL的情况下,在流动过程中,在所有链排列成向列相液晶相之前,在相对较低的剪切速率下就会形成织构。半刚性链之间的静电排斥会诱导链之间的相关性,在施加低应力时,在水中形成静电假凝胶,在0.01 M NaCl中形成的则较为松散。据我们所知,这是首次观察到这种行为。在0.1 M NaCl中,DNA的行为类似于相应的中性聚合物,这正如过量盐中的聚电解质所预期的那样,表现出屈服应力。当织构出现在水和0.01 M NaCl中时,在流变学曲线中观察到一个临界转变,在给定的临界剪切应力下粘度急剧下降,这与蠕变瞬态实验中也观察到的(γ˙)图中的平台期相对应。