Questions? Call 888-624-8373

PAPERBACK
list:$21.00
Web:$18.90
add to cart

Rights & Permissions

Free PDF Access

topleft topright

Opportunities to Improve Airport Passenger Screening with Mass Spectrometry (2004)
National Materials Advisory Board (NMAB)

Page
36
bottomleft bottomright

The following HTML text is provided to enhance online readability. Many aspects of typography translate only awkwardly to HTML. Please use the page image as the authoritative form to ensure accuracy.


Opportunities to Improve Airport Passenger Screening with Mass Spectrometry

FIGURE A-1 The resolution of two peaks in an IMS spectrum depends on the separation of their drift times and the width of the peaks at half intensity. An important quantity that governs whether two different substances are distinguishable by the drift time is the width of the intensity peaks. This width is quantified by wh, the width at half the maximum height of the distribution. Two drift times, td1 and td2, are distinguishable if |td1td2| > 1/2 (wh1 + wh2).

(For chromatographic devices, another common measure of device capability is the number of theoretical plates, N, which is related to the resolution by R = (N/5.55)1/2. The number of theoretical plates is often reported as a constant.)

This general expression for Pinf is easily extended to devices for which multiple parameters can be varied—e.g., for two parameters, x and y:

where it is assumed here that the resolution for y does not depend upon the value of x.

For ion mobility spectrometry (IMS), the output is the intensity and the variable parameter (x) is the drift time. The critical quantities, then, are the resolution of the drift time and the precision of the intensity measurements. The resolution of the drift time quantifies the degree of separation required to distinguish different peaks. At drift time t, the resolution is given by R(t) = t/wh(t), where wh(t) is the width of the peak at half maximum intensity, as shown in Figure A-1. (See, for example, Asbury and Hill, 1999; Matz, Tornatore, and Hill, 2001; Clemmer and Jarrold, 1997; Dugourd, Hudgins, Clemmer, and Jarrold, 1997.) The literature supports the assumption that the drift time resolution is constant, R(t) ≡ R. Matz et al. report that R is about 30 for commercial IMS instruments and use R = 36 in their calculations. Asbury and Hill report that for a typical IMS device, the number of theoretical plates rarely exceeds N = 5,000, which corresponds to R = 30.

The number of intensity values that can be reported, S, is also constant. Fetterolf and Yost use S = 212 for mass spectrometry. For IMS, the value of S appears to be less well defined. Often a 12-bit analog-to-digital converter is used, which would imply S = 212 at first glance. However, in practice the number of reproducible intensity values is much less, perhaps as low as 24 (Knapp 2003).

Page
36