Samalikova Maria, Grandori Rita
Institute of Chemistry, Johannes Kepler University, Altenbergerstrasse 69, 4040 Linz, Austria.
J Am Chem Soc. 2003 Nov 5;125(44):13352-3. doi: 10.1021/ja037000u.
According to a current model for protein electrospray, the charge-state distributions (CSDs) observed by electrospray-ionization mass spectrometry (ESI-MS) are controlled by the Rayleigh-limit charge of the droplets that generate the gas-phase protein ions. A testable prediction of this model is that the maximum charge state displayed by proteins in ESI-MS should respond to changes in the surface tension of the ESI droplets according to the Rayleigh equation. In this work, we subject this specific hypothesis to direct experimental testing. We show data obtained by time-of-flight (TOF) nano-ESI-MS with several different proteins in aqueous solutions containing 20-50% 1-propanol or 40% 1,2-propylene glycol. Both of these compounds have lower vapor pressure and lower surface tension than water. Propylene glycol also has a lower evaporation rate than water, providing an even more stringent test for surface tension effects in late ESI droplets. None of these cosolvents affects the CSDs of either folded or unfolded proteins as predicted by the Rayleigh-charge model. The only changes induced by 1-propanol can be ascribed to protein unfolding triggered above critical concentrations of the alcohol. Below such a threshold, no shift of the CSDs toward lower charge states is observed. The presence of 40% propylene glycol in the original protein solutions gives rise to CSDs that either are the same as those in the control samples or present much smaller changes than those calculated by the Rayleigh equation. Thus, the charge states of gas-phase protein ions produced by electrospray do not seem to be limited by the surface tension of the solvent. They rather appear to be quite protein-specific.
根据当前的蛋白质电喷雾模型,通过电喷雾电离质谱法(ESI-MS)观察到的电荷态分布(CSD)由产生气相蛋白质离子的液滴的瑞利极限电荷控制。该模型的一个可测试预测是,ESI-MS中蛋白质显示的最大电荷态应根据瑞利方程响应ESI液滴表面张力的变化。在这项工作中,我们对这一特定假设进行了直接实验测试。我们展示了通过飞行时间(TOF)纳米ESI-MS获得的数据,该实验使用了几种不同的蛋白质,这些蛋白质溶解于含有20%-50% 1-丙醇或40% 1,2-丙二醇的水溶液中。这两种化合物的蒸气压和表面张力都比水低。丙二醇的蒸发速率也比水低,这为ESI后期液滴中的表面张力效应提供了更严格的测试。这些共溶剂均未如瑞利电荷模型所预测的那样影响折叠或未折叠蛋白质的CSD。1-丙醇引起的唯一变化可归因于在高于酒精临界浓度时引发的蛋白质解折叠。在这样的阈值以下,未观察到CSD向较低电荷态的偏移。原始蛋白质溶液中40%丙二醇的存在导致CSD与对照样品相同,或者变化比根据瑞利方程计算的小得多。因此,电喷雾产生的气相蛋白质离子的电荷态似乎不受溶剂表面张力的限制。它们似乎相当具有蛋白质特异性。