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首页> 外文期刊>Biochimica et biophysica acta. Biomembranes >Glutamate, water and ion transport through a charged nanosize pore
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Glutamate, water and ion transport through a charged nanosize pore

机译:谷氨酸,水和离子通过带电纳米孔传输

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The transport of transmitter, ions and water through a positively-charged nanopore was investigated through computer simulations. The physics of the problem is described by a coupled set of Poisson-Nemst-Planck and Navier-Stokes equations in a computational domain consisting a cylindrical pore, whose radius ranged from 1 to 8nm and which was flanked by two compartments representing the vesicular interior and extra-cellular space. The concentration of co-ions is suppressed and of counter-ions enhanced, especially near the pore wall owing to electrostatic interactions. Glutamate (i.e. the transmitter considered) is negatively charged and is simulated as a counter-ion. The electro-kinetically induced pressure due to the movement of ions is negative and very pronounced near the pore wall where the concentration and flux of counter-ions is very high. The water velocity peaks in the pore center, diminishes to zero at the pore wall, but is constant along the pore axis. The mean velocity of the water/fluid is proportional to the vesicular pressure and pore cross-sectional area. Interestingly it is inversely related to the vesicular glutamate concentration. The factors determining the glutamate flux are complex. The diffusive flux generally predominates for narrow pore, and convective flux may dominate for wide pore if the vesicular pressure is high. Surprisingly at low vesicular pressure the mean total glutamate flux per unit cross-sectional pore area is higher for narrow pores. Higher flux is probably due to the rise of glutamate concentration in the nanopore, which is much more pronounced for narrow nanopores, due to the maintenance of approximate neutrality of charges in the pore and on the pore wall. In conclusion infra-vesicular pressure helps `flushing-out' the transmitter, but the induced pressure `drags-out' the water into the extra-cellular space. (c) 2006 Elsevier B.V All rights reserved.
机译:通过计算机模拟研究了传输器,离子和水通过带正电的纳米孔的传输。这个问题的物理原理是在计算域中由一组Poisson-Nemst-Planck方程和Navier-Stokes方程组耦合而成的,该方程域由一个圆柱孔构成,其半径范围为1至8nm,两侧是代表水泡内部和细胞外空间。由于静电相互作用,尤其是在孔壁附近,共离子的浓度被抑制并且反离子的浓度被增强。谷氨酸盐(即所考虑的发射器)带负电,并被模拟为抗衡离子。由于离子运动而产生的电动势是负的,并且在抗衡离子的浓度和通量非常高的孔壁附近非常明显。水速度在孔中心达到峰值,在孔壁处减小为零,但沿孔轴恒定。水/流体的平均速度与囊泡压力和孔截面积成正比。有趣的是,它与水泡谷氨酸浓度成反比。决定谷氨酸通量的因素很复杂。如果囊泡压力高,扩散通量通常主要用于狭窄的孔,而对流通量可能主要用于宽孔。出乎意料的是,在低水泡压力下,狭窄毛孔的每单位横截面孔面积的平均总谷氨酸通量更高。较高的通量可能是由于纳米孔中谷氨酸盐浓度的升高,这对于窄的纳米孔而言更为明显,这是由于维持了孔中和孔壁上电荷的近似中性。总之,囊泡下压力有助于“冲洗”变送器,但感应压力将水“抽吸”到细胞外空间。 (c)2006 Elsevier B.V保留所有权利。

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