School of Physics and Astronomy, University of Leeds, Leeds, UK.
Integr Biol (Camb). 2009 Feb;1(2):205-11. doi: 10.1039/b815601h. Epub 2008 Dec 11.
This work demonstrates the use of deep UV micropatterned chlorotrimethylsilane (TMS) monolayers to support lipid membranes on SiO(2) surfaces. After immersing such a patterned surface into a solution containing small unilamellar vesicles of egg PC, supported bilayer lipid membranes were formed on the hydrophilic, photolyzed regions and lipid monolayer over the hydrophobic, non-photolyzed regions. A barrier between the lipid monolayer and bilayer regions served to stop charged lipids migrating between the two. This allows the system to be used to separate charged lipids or proteins by electrophoresis. Either oppositely charged fluorescence labeled lipids [Texas Red DHPE (negative charge) and D291 (positive charge)] or lipids with different charge numbers [Texas Red DHPE (one negative charge) and NBD PS (two negative charges)] can be separated. We have also studied the migration of streptavidin attached to a biotinylated lipid. Negatively charged streptavidin responds to the applied electric field by moving in the direction of electroosmotic flow, i.e. towards the negative electrode. However the direction of streptavidin movement can be controlled by altering the difference in zeta potential between that of the streptavidin (zeta(1)) and the lipid membrane (zeta(2)). If zeta(1) > zeta(2), streptavidin moves to the negative electrode, while if zeta(1) < zeta(2), streptavidin moves to the positive electrode. This balance was manipulated by adding positively charged lipid DOTAP to the membrane. After measuring the average drift velocity of streptavidin as a function of DOTAP concentration, the point where zeta(1) approximately zeta(2) was found. At this point zeta(1) was calculated to be -9.8 mV which is in good agreement with the value of -13 mV from force measurements and corresponds to a charge of -2e per streptavidin, thus demonstrating the applicability of this method for determining protein charge.
这项工作展示了如何使用深紫外微图案化氯三甲基硅烷 (TMS) 单层来支持二氧化硅 (SiO2) 表面上的脂质膜。将这种图案化表面浸入含有小单层卵磷酯 (PC) 囊泡的溶液中后,亲水性、光解区域上形成了支撑双层脂质膜,而疏水性、非光解区域上则形成了脂质单层。脂质单层和双层区域之间的屏障可以阻止带电脂质在两者之间迁移。这使得该系统可用于通过电泳分离带电脂质或蛋白质。可以分离带相反电荷的荧光标记脂质[Texas Red DHPE(负电荷)和 D291(正电荷)]或带有不同电荷数的脂质[Texas Red DHPE(一个负电荷)和 NBD PS(两个负电荷)]。我们还研究了连接在生物素化脂质上的链霉亲和素的迁移。带负电荷的链霉亲和素会对施加的电场做出反应,朝着电渗流的方向(即负电极)移动。然而,通过改变链霉亲和素(ζ1)和脂质膜(ζ2)之间的 ζ 电位差,可以控制链霉亲和素的运动方向。如果 ζ1 > ζ2,链霉亲和素移动到负电极,而如果 ζ1 < ζ2,链霉亲和素移动到正电极。通过向膜中添加带正电荷的脂质 DOTAP 来操纵这种平衡。在测量链霉亲和素作为 DOTAP 浓度函数的平均漂移速度后,找到了 ζ1 约等于 ζ2 的点。此时,ζ1 计算为 -9.8 mV,这与力测量得出的 -13 mV 值非常吻合,对应于每个链霉亲和素的电荷为 -2e,从而证明了这种方法用于确定蛋白质电荷的适用性。