How to Identify Molecules - Proton NMR: Crash Course Organic Chemistry #26 - By Math and Science
Transcript
00:0-1 | You can review content from Crash course Organic Chemistry with | |
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00:05 | devices . Hi , I'm dave okay Chakravarty and welcome | |
00:08 | to Crash course Organic chemistry chemists used to have a | |
00:11 | real problem when it came to identifying the crystals liquid | |
00:15 | or general group they found themselves with at the end | |
00:18 | of a chemical reaction . Of course they knew what | |
00:21 | they were trying to make . But have they actually | |
00:24 | made it ? They could check boiling points , melting | |
00:26 | points , smell color or even taste in the bad | |
00:30 | old days , which is definitely not recommended now . | |
00:33 | But all of that took weeks of diligent effort and | |
00:36 | was still somewhat inconclusive , fortunately we've moved on to | |
00:39 | a much more high tech analytical technique , nuclear magnetic | |
00:43 | resonance or NMR Yeah . Mhm Yeah . First off | |
00:56 | let's straighten one thing out . The nuclear part of | |
00:58 | any mars name doesn't refer to nuclear power . It | |
01:01 | refers to the nuclei of atoms . All atomic nuclei | |
01:04 | are made up of protons and neutrons except for hydrogen | |
01:07 | , which doesn't have any neutrons adding up the protons | |
01:10 | and neutrons gives us the atoms mass number . Nuclei | |
01:13 | with odd mass numbers have a property called spin and | |
01:16 | having spin makes them observable using NMR . Obviously there | |
01:19 | are quite a lot of elements with odd mass numbers | |
01:22 | , but we're only interested in a handful of them | |
01:24 | for NMR nitrogen 15 flooring 19 , phosphorus 31 . | |
01:28 | I'll show up occasionally , but the real stars are | |
01:31 | carbon 13 and hydrogen . We'll focus on hydrogen today | |
01:34 | and do proton NMR spin is not the nuclei literally | |
01:38 | spinning . It's one of those weird quantum mechanical things | |
01:41 | to avoid getting too into the physics , we'll just | |
01:43 | say that when charged particles like protons in a nucleus | |
01:46 | move , a magnetic field with the magnetic moment is | |
01:49 | created . If you've played with iron filings before , | |
01:51 | you know , they move if you put a magnet | |
01:53 | near them , each iron filing has a magnetic moment | |
01:57 | and under normal circumstances there directions are random . However | |
02:01 | , in the presence of a magnet which has a | |
02:02 | magnetic field , they all line up similarly , if | |
02:06 | you stick a nucleus with a magnetic moment in an | |
02:08 | external magnetic field , it either lines up with that | |
02:11 | field or exactly against it . It takes less energy | |
02:14 | to align with the magnetic field and more energy to | |
02:17 | go against it . So there's a clear energy difference | |
02:20 | between the two different spin states . Now we've got | |
02:22 | the nuclear and magnetic parts of NMR covered . But | |
02:26 | what about the resonance ? It turns out that particular | |
02:28 | frequencies of radio waves will cause the nuclei to flip | |
02:31 | from one spin state to the other when we hit | |
02:34 | that perfect frequency . That's what we call resonance . | |
02:37 | And the nuclei absorb the energy of the radio waves | |
02:40 | . This is we are a detector , measures the | |
02:42 | frequency and intensity of the radio wave that got absorbed | |
02:45 | and plots it on a spectrum . In this episode | |
02:48 | , we're going to concentrate on proton NMR , which | |
02:50 | tells us about the hydrogen nuclei and therefore hydrogen atoms | |
02:54 | in molecules in general will get a huge magnet and | |
02:57 | dissolve our chemical sample in a special decorated solvent where | |
03:01 | the hydrogen atoms are replaced by deuterium . If we | |
03:04 | used a regular old solvent with protons , the signals | |
03:06 | from our organic chemical would be overwhelmed by the hydrogen | |
03:09 | is on all the solvent molecules . Then we put | |
03:11 | our tiny solution of chemical sample in the middle of | |
03:14 | the magnet blast a pulse of radio waves and measure | |
03:17 | the energy released by the nuclei as the different hydrogen | |
03:19 | atoms in the chemical go from residents back to their | |
03:22 | ground state . Like IR spectroscopy that we talked about | |
03:25 | in episode five , we get a spectrum from the | |
03:27 | sample . Once we look at some proton NMR spectra | |
03:30 | will get the hang of these patterns . Let's start | |
03:33 | with a simple example . This is the spectrum for | |
03:35 | chloroform , ethyl methyl ether or mom chloride to its | |
03:38 | friends . The X axis is measured in PPM , | |
03:41 | which stands for parts per million . It has to | |
03:43 | do with the ratio between the radio frequency source and | |
03:46 | the energy required to cause the nuclei to flip spin | |
03:49 | . The process of adding deuterium to solvents isn't perfect | |
03:52 | . So a few hydrogen is from the NMR solvent | |
03:55 | show up as a peak , which we can use | |
03:57 | to set the scale of our NMR spectrum . Or | |
04:00 | we can include a standard chemical called tetra metal silent | |
04:03 | or TMS in the sample , which produces a very | |
04:06 | strong signal . TMS shows up on the far right | |
04:09 | of the spectrum and usually doesn't overlap with the peaks | |
04:11 | from the hydrogen is on our organic chemical basically , | |
04:14 | the standard provides a comparison point for the other peaks | |
04:17 | . It's a bit like measuring times against GMT . | |
04:20 | If you live in new york , your time zone | |
04:22 | is gmt minus five . While someone in paris is | |
04:25 | on GMt plus one and someone in Canberra Australia is | |
04:28 | on GMT plus 11 . So ignoring the peak at | |
04:31 | zero from our tMS standard , there are only two | |
04:34 | peaks we need to analyze in the spectrum . Using | |
04:37 | a computer , we can label each of these peaks | |
04:39 | with the integral the area underneath them , which corresponds | |
04:43 | to the ratio of the number of protons in that | |
04:45 | part of the molecule . One of our peaks here | |
04:47 | has an integral value of three , which means three | |
04:49 | protons . So that means there's probably a medical group | |
04:52 | , CH three in our sample . The other peak | |
04:54 | has an integral of two , which suggests our chemical | |
04:57 | also contains a CH two groups . So if we | |
04:59 | were a chemist in the lab who didn't know but | |
05:01 | just suspected that we had mom chloride , we could | |
05:04 | check whether the structure of our suspected molecule fits with | |
05:07 | our spectrum . And , yep , there sure is | |
05:10 | a CH three and CH two groups in mom chloride | |
05:13 | . One of the peaks is upfield or further to | |
05:15 | the right and the other is more downfield or further | |
05:18 | to the left . That's because the protons making up | |
05:20 | these peaks are surrounded by different amounts of electrons because | |
05:24 | of different neighboring atoms . Nearby electrons from other atoms | |
05:27 | can shield the proton nuclei from the magnetic field so | |
05:30 | they feel it less . And we need a lower | |
05:32 | frequency radio wave to flip the spin . On the | |
05:35 | other hand , electro negative atoms can draw electrons away | |
05:38 | from proton nuclei . So there d shielded feel the | |
05:40 | magnetic field more and need a higher frequency radio wave | |
05:44 | to flip the spin . Taking a look at mom | |
05:46 | chloride , we can see the CH three group is | |
05:47 | attached to an electro negative element oxygen , but the | |
05:51 | CH two group is sandwiched between two electro negative atoms | |
05:54 | and oxygen and chlorine . So the electrons near the | |
05:57 | CH two groups are more drawn away . The proton | |
06:00 | nuclei are more D . Shielded and the peak is | |
06:03 | down field of the CH three groups . To keep | |
06:05 | it really simple , Just remember that the presence of | |
06:07 | electro negative atoms or groups . She speaks to the | |
06:10 | left in proton NMR . The peaks on the spectrum | |
06:13 | actually a pretty consistent shifts based on the electro negativity | |
06:16 | and hybridization of the atoms near the protons tables like | |
06:20 | this . Can't cover every possibility though , which is | |
06:23 | why we need to understand how to think about electro | |
06:25 | negativity and chemical shift . Okay , now that we've | |
06:28 | talked through the mom chloride spectrum , let's try another | |
06:32 | example . This is the proton NMR spectrum of ethanol | |
06:35 | . There are three peaks in this one , but | |
06:38 | two of them are more like groups of lines . | |
06:40 | There are lots of protons in organic molecules and remember | |
06:44 | that each nucleus with an odd mass number has been | |
06:47 | and a magnetic moment . So protons on one carbon | |
06:51 | can influence protons on an adjacent carbon in a process | |
06:54 | called coupling , this leads to the split peaks or | |
06:57 | groups of lines that we're seeing here . In fact | |
06:59 | , this has been observed so regularly that we can | |
07:02 | predict how many times a peak will be split . | |
07:05 | Thanks to the aptly named N plus one rule , | |
07:07 | we know that a peak will be split N plus | |
07:09 | one times where N . Is the number of protons | |
07:12 | on adjacent carbons . The best way to understand splitting | |
07:15 | is by looking at examples . So let's start with | |
07:18 | our most shielded peak . It's at about one PPm | |
07:21 | with an integral of three . So we know it's | |
07:23 | the CH three group , were still practicing . So | |
07:26 | let's look at the structure of ethanol . The CHD | |
07:29 | group is bonded to a CH two group . There | |
07:31 | are two protons on the neighboring carbon that are coupled | |
07:34 | . This means N . Is to using the N | |
07:36 | plus one rule , we can do two plus one | |
07:38 | equals three . So the CH three peak should be | |
07:41 | split into three . Now going one peak downfield at | |
07:44 | about three PPm . We see the CH two groups | |
07:47 | in our spectrum . It's down field of the CH | |
07:49 | three because the CH two group is bonded to an | |
07:51 | electro negative oxygen atom in the structure of ethanol . | |
07:54 | We know that the CH two group is bonded to | |
07:56 | the CH three group . So there are three protons | |
07:59 | on the neighboring carbon that are coupled and N . | |
08:02 | Is three . Using the N . Plus one . | |
08:04 | Rule three plus one equals four . So the CH | |
08:07 | two peak is split into four plus . It has | |
08:10 | an integral of two , telling us there are two | |
08:12 | protons . The split peak patterns , or multiplicity is | |
08:15 | have special names too . The ch the peak split | |
08:18 | into three is a triplet , and the CH two | |
08:20 | peak split into four is a quartet . The third | |
08:22 | peak at about four PPm is the proton on the | |
08:25 | O . H . Group of our ethanol molecule . | |
08:27 | O . H . Protons are tricky because they can | |
08:29 | swap with other protons in the sample solution and can | |
08:31 | turn up as a new split peaks pretty much anywhere | |
08:34 | in the spectrum . In fact , sometimes they don't | |
08:37 | show up at all . It's also important to mention | |
08:39 | that the protons on oxygen and nitrogen don't split the | |
08:42 | protons on adjacent carbons . So these protons don't count | |
08:46 | when figuring out N plus one . After you look | |
08:48 | at more peaks and more spectra solving these logic puzzles | |
08:51 | can be fun . And because the whole point of | |
08:53 | proton NMR is to figure out the structure of molecules | |
08:56 | . This next spectrum doesn't come with a name , | |
08:58 | structure like mom chloride or ethanol , fortunately , we | |
09:02 | have a high resolution mass spectrum that gives us our | |
09:04 | chemical formula C five H 802 So let's start with | |
09:08 | the most shielded part of the spectrum . We have | |
09:11 | two single peaks that have integral of three protons each | |
09:15 | . So it looks like we have two ch three | |
09:17 | groups on our mystery molecule . Next we can see | |
09:19 | that the most d shielded single peak has an integral | |
09:22 | of one proton . Referring back to our handy chart | |
09:24 | . we can see this is where the proton on | |
09:26 | a carb oxalic acid shows up . And what do | |
09:29 | you know ? We have two oxygen atoms in our | |
09:31 | formula which fits perfectly with that thought , let's add | |
09:34 | this fragment to the pieces of our molecule , puzzle | |
09:36 | one more peek to go and this single peak corresponding | |
09:40 | to one proton is a bit D . Shielded to | |
09:42 | . In fact looking at our chart again , it's | |
09:45 | showing up in the range of alkaline hydrogen atoms . | |
09:47 | The trickiest part about putting these four pieces together is | |
09:50 | figuring out where to place the two methyl groups and | |
09:52 | the car back silic acid on . Are all keen | |
09:54 | to start . Let's put the two ch three groups | |
09:57 | on different sides of the alkaline . Wait a second | |
09:59 | though , with this structure of the metal group is | |
10:01 | next to a carbon atom with the hydrogen . This | |
10:04 | would split a single peek into a doublet and we'd | |
10:06 | expect the hydrogen atom to be split by the three | |
10:08 | hydrogen on the metal to since we don't see splitting | |
10:12 | in the spectrum , let's rearrange our structure . So | |
10:14 | the hydrogen atom and both metal groups won't be split | |
10:17 | by any adjacent protons , even though the two methyl | |
10:20 | groups are attached to the same carbon double bonds are | |
10:23 | rigid , so one of these groups is stuck on | |
10:25 | the same side as the car back , silic acid | |
10:27 | and one is on the same side as the hydrogen | |
10:29 | . These metal hydrogen Zarin different chemical environments and they're | |
10:33 | not chemically equivalent . So that's why they show up | |
10:35 | as two different peaks . We'll talk more about chemical | |
10:38 | equivalents in a later episode , when we look at | |
10:40 | the proton and um are spectra of aromatic compounds . | |
10:43 | But in this episode we've learned nuclear magnetic resonance helps | |
10:46 | us visualize the atoms in molecules as peaks in the | |
10:49 | spectrum . In proton NMR . The integral tells us | |
10:52 | how many hydrogen each peak represents nuclei close to electro | |
10:56 | negative atoms appear downfield on a spectrum and split peaks | |
11:00 | or multiplicity give clues about how atoms are joined to | |
11:03 | other atoms . In the next episode will work our | |
11:06 | way through reactions of some other often fragrant compounds Aldo | |
11:09 | hides and key tones . Until then , Thanks for | |
11:12 | watching this episode of Crash Course Organic Chemistry . If | |
11:15 | you want to help keep all Crash Course free for | |
11:17 | everybody forever , you can join our community on Patreon | |
11:23 | . Yeah . |
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