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MASS SPECTROMETRY

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MASS SPECTROMETRY

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Mass spectrometry (MS) is an analytical technique that ionizes chemical species and sorts 

the ions based on their mass-to-charge ratio. In simpler terms, a mass spectrummeasures the 

masses within a sample. Mass spectrometry is used in many different fields and is applied to 

pure samples as well as complex mixtures.

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A mass spectrum is a plot of the ion signal as a function of the mass-to- charge ratio. These spectra are used to determine the elemental or 

isotopic signature of a sample, the masses of particles and of molecules,  and to elucidate the chemical structures of molecules and other 

chemical compounds.

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In a typical MS procedure, a sample, which may be solid,  liquid, or gas, is ionized, for example by bombarding it with  electrons. This may cause some of the sample's 

molecules to break into charged fragments. These ions  are then separated according to their mass-to-charge 

ratio, typically by accelerating them and subjecting them to  an electric or magnetic field: ions of the same mass-to-

charge ratio will undergo the same amount of deflection.

[1]

 

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The basic principle

If something is moving and you subject it to a sideways  force, instead of moving in a straight line, it will move in a  curve - deflected out of its original path by the sideways  force.

Suppose you had a cannonball travelling past you and you 

wanted to deflect it as it went by you. All you've got is a jet 

of water from a hose-pipe that you can squirt at it.

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But suppose instead, you tried to deflect a table tennis ball 

travelling at the same speed as the cannonball using the 

same jet of water. Because this ball is so light, you will get 

a huge deflection.

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The amount of deflection you will get for a given sideways 

force depends on the mass of the ball. If you knew the 

speed of the ball and the size of the force, you could 

calculate the mass of the ball if you knew what sort of 

curved path it was deflected through. 

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The less the deflection, the  heavier the ball.

You can apply exactly the same

principle to atomic sized particles.

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