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In a time-of-flight mass spectrometer if $q$ is the charge and $m$ the mass of the ionized species, then the time of flight is proportional to

  1. $\frac{\sqrt m}{\sqrt q}$
  2. $\frac{\sqrt q}{\sqrt m}$
  3. $\frac{m}{\sqrt q}$
  4. $\frac{q}{\sqrt m}$
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