09.12.2012 Views

Mass Spectrometry A Textbook - Department of Mathematics and ...

Mass Spectrometry A Textbook - Department of Mathematics and ...

Mass Spectrometry A Textbook - Department of Mathematics and ...

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

11.3 Ion Formation 453<br />

field strength is impossible. Instead, at the moment the critical electric field<br />

strength is reached, the Taylor cone instantaneously forms <strong>and</strong> immediately starts<br />

ejecting a fine jet <strong>of</strong> liquid from its apex towards the counter electrode. [64] This<br />

mode <strong>of</strong> operation is termed cone-jet mode. [5] The jet carries a large excess <strong>of</strong><br />

ions <strong>of</strong> one particular charge sign, because it emerges from the point <strong>of</strong> highest<br />

charge density, i.e., from the cone's tip. However, such a jet cannot remain stable<br />

for an elongated period, but breaks up into small droplets. Due to their charge,<br />

these droplets are driven away from each other by Coulombic repulsion. Overall,<br />

this process causes the generation <strong>of</strong> a fine spray, <strong>and</strong> thus gave rise to the term<br />

electrospray (Figs. 11.11 <strong>and</strong> 11.12).<br />

11.3.2 Disintegration <strong>of</strong> Charged Droplets<br />

When a micrometer-sized droplet carrying a large excess <strong>of</strong> ions <strong>of</strong> one particular<br />

charge sign – some 10 4 charges are a realistic value – evaporates some solvent, the<br />

charge density on its surface is continuously increased. As soon as electrostatic<br />

repulsion exceeds the conservative force <strong>of</strong> surface tension, disintegration <strong>of</strong> the<br />

droplet into smaller sub-units will occur. The point at which this occurs is known<br />

as Rayleigh limit. [38] Originally, it has been assumed that the droplets would then<br />

suffer a Coulomb fission (or Coulomb explosion). This process should occur repeatedly<br />

to generate increasingly smaller microdoplets. While the model <strong>of</strong> a cascading<br />

reduction in size holds valid, more recent work has demonstrated that the<br />

microdroplets do not explode, but eject a series <strong>of</strong> much smaller microdroplets<br />

from an elongated end (Fig. 11.13). [49,79,80] The ejection from an elongated end<br />

can be explained by deformation <strong>of</strong> the flying microdroplets, i.e., they have no<br />

Fig. 11.13. Illustration <strong>of</strong> droplet jet fission. The average number <strong>of</strong> charges on a droplet,<br />

the radii <strong>of</strong> the droplets [µm], <strong>and</strong> the timescale <strong>of</strong> events are assigned. The inset shows a<br />

drawing <strong>of</strong> droplet jet fission based on an actual flash microphotograph. Reproduced from<br />

Ref. [49] by permission <strong>of</strong> the authors.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!