Introduction

A time-of-flight mass spectrometer uses the differences in transit time through a drift region to separate ions of different masses. It operates in a pulsed mode so ions must be produced or extracted in pulses. An electric field accelerates all ions into a field-free drift region with a kinetic energy of qV, where q is the ion charge and V is the applied voltage. Since the ion kinetic energy is 0.5mv2, lighter ions have a higher velocity than heavier ions and reach the detector at the end of the drift region sooner.
 
 

Theory:

          K.E. = qV

          1/2 mv2 = qV

          v = (2qV/m)1/2

The transit time (t) through the drift tube is L/v where L is the length of the drift tube.

          t=L / (2V/m/q)1/2
 
 

Instrumentation

Schematic of a linear TOF-MS

This schematic shows ablation of ions from a solid sample with a pulsed laser. The reflectron is a series of rings or grids that act as an ion mirror. This mirror
compensates for the spread in kinetic energies of the ions as they enter the drift region and improves the resolution of the instrument. The output of an ion
detector is displayed on an oscilloscope as a function of time to produce the mass spectrum.