Fernandez de la Mora Juan
Department of Mechanical Engineering and Materials Science, Yale University, 9 Hillhouse Avenue, PO Box 8286, New Haven, CT, 06520-8286, USA.
J Am Soc Mass Spectrom. 2019 Jun;30(6):1082-1091. doi: 10.1007/s13361-019-02171-0. Epub 2019 Apr 9.
We study the space charge limited maximal current density j″ of mobility-selected ions that can be transmitted in ion mobility spectrometry (IMS). Theory and experiments focus on differential mobility analyzers (DMAs), but are readily generalizable to other IMS devices. Repulsion between the ions in the cloud leads to beam spreading, with significant broadening once the ion number density n becomes comparable to the space charge saturation limit n = εE/(eΔ). Δ is the distance traversed by the ions in the direction of an externally imposed electric field E, and e is the charge on each ion. For ions of electrical mobility Z, j″ is then limited below j″ = ZEen = ZεE/Δ. A theory including diffusion and space charge effects is developed that reduces to Burgers' exactly solvable equation. The theory is tested in experiments with room temperature electrosprays (ES) of 100 mM [ethylN-formate] in methanol. This spray produces primarily a single ionic species at very high initial concentration n, which may be tuned above or below n by varying the distance from the ES emitter to the inlet slit of the DMA. Mobility-selected ion densities n > 3.10 ions/cm are achieved, with n~n, and with drastically broadened mobility peak shapes having the approximate top hat-predicted shapes. However, the largest n values approaching n are not quantitatively measurable because the densest sprays do not fill the outlet slit length. Graphical Abstract .
我们研究了在离子迁移谱(IMS)中能够传输的迁移率选择离子的空间电荷限制最大电流密度j″。理论和实验主要关注差分迁移率分析仪(DMA),但很容易推广到其他IMS设备。离子云中离子之间的排斥导致束流扩散,一旦离子数密度n与空间电荷饱和极限n = εE/(eΔ)相当,就会出现显著展宽。Δ是离子在外部施加电场E方向上穿过的距离,e是每个离子的电荷量。对于电迁移率为Z的离子,j″则被限制在j″ = ZEen = ZεE/Δ以下。我们发展了一种包含扩散和空间电荷效应的理论,该理论简化为伯格斯可精确求解的方程。该理论在室温下以甲醇中100 mM [甲酸乙酯]的电喷雾(ES)进行的实验中得到了验证。这种喷雾在非常高的初始浓度n下主要产生单一离子物种,通过改变从ES发射器到DMA入口狭缝的距离,可以将其调至高于或低于n。实现了迁移率选择离子密度n > 3.10离子/cm,n约等于n,并且迁移率峰形状大幅展宽,具有近似礼帽预测的形状。然而,接近n的最大n值无法进行定量测量,因为最密集的喷雾无法充满出口狭缝长度。图形摘要 。