Hey everyone. So mass spectrometry involves the ionization, the separation, and finally the detection of gaseous ions according to their mass to charge ratios. So, let's say that we're starting out with the sample and let's say that this sample is just m. We don't know what its phase is; it could be a liquid, gas, or solid. And because we don't know the phase, we can say that before we get to the ionization step, there's actually one step before it, and that is the vaporization step. So, we're going to say step 1 is vaporization. Let's assume that this unknown compound M is a liquid. Vaporizing it, we change it into a gas. So now, it's a gas and it's gone through step 1.
Once it's gotten through step 1, it goes into step 2, where it enters an ionization chamber. In this ionization chamber, we bombard this compound with a single electron. We hit it so hard with this single electron that it knocks off an electron from it. Remember, electrons come in pairs. We've lost 1 electron, so you're plus 1, and we still have that other electron that's unpaired now. This creates what we call a radical cation. Remember, radical is when you have an unpaired electron. It's a cation because it's positive. We could also refer to this cation, this radical cation also as our parent ion or our molecular ion. It represents our unknown compound where it's just lost one electron.
From there, it enters into an acceleration phase, so this is step 3. Basically, here it's being accelerated through the use of electrical fields. Because we have a charge on it, it can be influenced by those electrical fields, which push it through to where it passes into here, and on both sides, we have electromagnets. These electromagnets help us enter into the 4th step, which is deflection. Now, the charged forms of this unknown compound are going to be deflected by this electrical field created by these electromagnets. But what we need to realize here is that there's not just one of this and one of this. There are hundreds of them, and a bunch of them are being bombarded by electrons, some of them becoming this radical cation, some of them not being hit by electrons and staying in their neutral form. Those that stay in their neutral form, they're not affected by the electromagnets. So, they themselves could crash into the walls on either side, and their progress stops. Those that possess a charge pass through, they're going to be curved by the magnetic field created by the electromagnets, and as a result, they wind up down here.
This final step is the detection step, and we're detecting it by it hitting, this basically is this ion counter here, or detector. Okay, so step 5 deals with detection by an ion counter. Now, this counter can be hooked up to a computer, and this computer picks all the fragments that are hitting this detector and it can craft what we call a mass spectrum. This mass spectrum gives us the most stable charged fragments that exist for this unknown compound. So here, we look at the highest peaks here. For the fragments, this one all the way down here represents the radical cation with its mass. So we can see that the mass of this unknown is above 110 grams per mole. We can also say that this peak that's highest up represents the most stable fragment, and this would be called our base peak.
Now, in conjunction with this piece of information and other types of what we call spectroscopic techniques, we can piece together what we think our unknown compound resembles. So mass spectrometry can help give us a big amount of clues in terms of what a compound could be, but usually, we don't use it alone. We use it with IR spectroscopy, NMR spectroscopy, as well as other types of techniques, that together can give us a more complete picture of our unknown compound. Just remember with mass spectrometry, we ionize a sample, we send it through a mass spectrometer. Through this, we are able to construct the basic mass, overall mass of our unknown compound.