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Nanotechnology-Enabled Sensors

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5.10 Mass Spectrometry 271<br />

beam experiences a strong magnetic field perpendicular to its direction, the<br />

ions are deflected in an arc whose radius is inversely proportional to the<br />

mass of the ion. Lighter ions are deflected more than heavier ions. By<br />

varying the strength of the magnetic field in time, ions of different masses<br />

impinge on a detector that is placed at the end of a curved tube at different<br />

times. 15<br />

Fig. 5.47 The Mass Spectrometry setup.<br />

Fig. 5.48 shows an example of a mass spectrum of a relatively simple<br />

carbon dioxide molecule, CO2. Mass spectra are generally presented as a<br />

graph having vertical bars, where each bar represents an ion having a specific<br />

mass-to-charge ratio (m/z) and the length of the bar indicates its relative<br />

abundance. The ion with the highest abundance is assigned to 100, and<br />

it is referred to as the base peak. CO2 has a nominal mass of 44 amu. As<br />

can be seen in Fig. 5.48, the molecular ion is the strongest ion in the CO2<br />

mass spectrum. Carbon dioxide’s mass spectrum is very simple, as its<br />

molecule is comprised of only three atoms. In this graph, the molecular ion<br />

is the base peak, and the only fragment ions are CO (m/z=28) and O<br />

(m/z=16).

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