Subtitles section Play video Print subtitles >> All right, well I think maybe we'll begin even if the last few people come in. So I want to talk about two related techniques today. They are related in pulse sequence. They're completely different in what they do. One of them is TOCSY and one of them is ROESY. So TOCSY is a correlation experiment. It stands for Total Correlation Spectroscopy. I'll put total in quotes because one doesn't get an infinite number of cross peaks. This technique was co-developed, developed at the same time with another technique that's the same pulse sequence called HOHAHA which always sounds good at Christmastime. It stands for Homonuclear Hartmann-Hahn Spectroscopy and they're the same technique but TOCSY has taken over, so the idea is that you get cross peaks with all and again I'm going to put this in quotes because there are limits, other spins in the spin system and so what this technique is like is it's like a super COSY. I mean, I'll give you a really simple example here. If we have propanol and that was sort of the sketch of the molecule when I gave the first [inaudible] in 2D spectra if you have propanol COSY will link your methyl group to your central methylene and it will link the central methylene to the next methylene and assuming the OH is exchanging rapidly that won't be linked in there. What TOCSY will do since all of these groups are in the same spin system is TOCSY will also link the methyl group to the terminal methylene and where TOCSY really, really shines, there are sort of two different situations that TOCSY really shines. In the small molecules realm where TOCSY really shines is in situations of overlap and I've been pretty good about giving you spectra where there's not too much overlap and you can walk your way through COSY but sometimes you'll end up with peaks overlapping on other peaks and you simply stop being able to walk your way through and so you look and you say, hey what's going on here I can't figure out my way all the way through, so I'll just give you a couple of hypothetical examples that maybe illustrate my thinking on this of a case where you might have overlap. So like if you take a molecule of pentanol and we think about where things typically show up at it we'd say all right plain vanilla methyl is.4 and methylene that's next to an oxygen say is at 3.5 parts per million and methylene that's beta to an oxygen that's going to be I don't know that's going to be somewhere around 1.9 parts per million but by the time you get down to this methylene chain-- bless you-- you're going to have your methylenes pretty much unperturbed both at about 1.4 ppm. In other words, if you go into the COSY spectrum you're going to get into a quagmire right here where you have trouble tracing your way through the COSY spectrum and so those types of issues, if you've got multiple spin systems in the molecule and you're really trying to figure out what your fragments are those types of issues can be problematic and so again let me give you a molecule and just sort of talk about typical chemical shifts, so if we'd say, all right an ester of methylene next to an ester, I usually think 4.1 ppm, plane vanilla methylenes I think about, methyls I think about 9 parts per million. A methyl group that's beta to a carbonyl I think about, say about 1.1 parts per million. In other words it's beta to an electron withdrawing group so it's at the plane position shifted down by a couple of tenth of a ppm but then if you think about a methine that's say beta to an oxygen, normally I think about a methine maybe at 1.9 ppm but by being beta to an oxygen maybe it will be about 2.4 ppm and normally I'll think of say a methyl group as next to an ester as being about 2 parts per million but if it's a methylene group it will go down by another about.4 parts per million so you could easily how a molecule like this might have two spin systems where when you try to trace your way through you get caught up and so if everything overlapped at 2.4 it would be really hard in a COSY of a molecule like this to distinguish this spin system from this one, in other words to try to walk your way through and see if this methyl was part of a different spin system than this methyl over here and TOCSY's extremely good at doing this. The other thing that TOCSY is good at, there's a parameter that's very important in TOCSY called the spin lock mixing time and so when I say all other spins in the spin system we're typically talking about within a limit maybe through about 7 bonds. If you vary the spin lock mixing time and you can use TOCSY as sort of a super COSY experiment where if you have a very short time you basically get just one jump just like from here to here but if you go a little longer two jumps starts to appear. If you go a little longer in your spin lock mixing time more and more go. So you can do a series of TOCSY experiments that will basically walk your way from one spin to the next to the next and what's good is if you have a region where there's overlap and then a region where there isn't overlap, so like the overlap might be at 2.4 in this molecule and the region that doesn't have overlap might be at say 1.1 and.9 you can go ahead and walk along those TOCSY tracks and see who the coupling partner is for each and then do longer and longer mixing times to pick them all out. So that's one really good use for TOCSY is overlap. The other really good use is I'll call it biopolymers which sounds like something intimidating but any sort of molecule that has spin systems that are units within, so there are many types of macro lactams and many types of antibiotic, cyclic esters that have unnatural amino acids that have a series of spin systems. I'll just show you some biopolymers for example, peptides and proteins and so if you think about it each amino acid in a peptide or a protein is its own spin system and so forth where each unit comprises a spin system and so you can pick out all of these spin systems and basically very quickly assign all of the resonances in a polypeptide and we'll do an example of this with a cyclic peptide. Sugars are another example. We just saw Professor Peng Wu's seminar and he was working with various types of oligosaccharides and so each oligosaccharide, each monosaccharide unit is an isolated unit and they're often very heavily overlapped and so I'm just giving sort of a generic cartoon of an oligosaccharide structure. And so each sugar unit is its own spin system and TOCSY they are very crowded together. They all end up having similar chemical shifts and TOCSY really shines at working with oligosaccharides. And the other area that works out very well with TOCSY is nucleic acids, DNA and RNA where again the basic unit is sugars and bases and each sugar is its own little spin system. And so you have a nuclear base and depending on if it's DNA or RNA you'll have an OH at these positions so I'll just put this in brackets. So again, all of these are representing kind of pieces of a biopolymer structure that might be useful for elucidating. [ Silence ] So as I was hinting at before, one of the limits of TOCSY is it doesn't go on forever and so the limits are I'm going to say, I always hate to put a hard number, about 7 bonds so for example, what do I mean? I mean let's say we look at the molecule lysine, so lysine is an amino acid with a four carbon chain. I'll put this as part of a biopolymer. So if you're talking about tracing your way from the epsilon carbon to the NH group you're going through one, two, three, four, five, six, seven bonds. That's about as far as you would go and so in other words you'd end up having this hydrogen, if you do it right, crossing with all of the methylenes along the way giving cross peaks as well as if you do right the NH group, unless you do the experiment in D2O in which case the NH group will have exchanged. So as I said the parameter is, the key parameter is a mixing time and typically this is one of the experiments, the experiments downstairs that are like a COSY experiment or an HMQC experiment or an HMBC experiment the parameters John Greaves gives you, if you take this default 10 hertz HMBC experiment that's going to be sort of one size fits all. In the case of a TOCSY experiment you actually have to think intelligently about the experiment. Typical values are about 75 to 100 millisecond spin lock mixing time and you'd obviously, you'd want to go to the high end to pick up longer correlations you might go up to say 200 milliseconds. If you go shorter, particularity if you're down sort of in the 25 to 75 range you'll be using the experiment as kind of a super COSY but one where you can walk your way from one bond to the next to the next. Now one of the implications for your own project is that with strychnine is because strychnine has some really extended spin systems you may not be able to trace your way through all of the spin systems but you'll be able to get part way. The other limitation, so obviously, so one limit is the number of bonds. The other limit is your coupling basically proceeds directly depending on how strongly things are coupled, in other words if you have a very small J that can lead to an absence of cross peaks so it's not so much an issue with a flexible chain but if you come down to strychnine and you're tracing your way through a spin system where one dihedral is close to 90 degrees. Your coupling constant is very small, a hertz or two or zero hertz. If you have a really small coupling constant TOCSY may not take you through. Basically, you need to have some reasonably large couplings, so you may see things behaving like as if they're isolated spin systems or nearly isolated spin systems so, now the nice thing about TOCSY as I said is it's very good at dealing with overlap and I'll show you in just a moment an example where you just would be struggling like crazy by COSY and we're going to assign a zillion different protons in one fell swoop. There's an alternative that's extremely powerful and we'll talk about it in the last week of class and that's the HMQC TOCSY. So TOCSY works as long as you can find some regions where there aren't overlap and you can get one resonance that isn't overlapping but if you've got really bad overlap you may even have trouble tracing your way through a TOCSY. HMQC TOCSY is a variant that's like TOCSY but it has the dispersion of the C 13 dimension. Remember C 13 resonance is because you have 200 ppm end up having very little overlap and so the dispersion can be very, very powerful. That's too much for us to assimilate at this point so let me just say I'll show you that in the future. All right, what I'd like to do now is to talk about, give us an example of one molecule. We're going to assign every resonance in this molecule and the molecule is gramicidin S. It's an antibiotic and it's a non-ribosomal peptide. What that means is that it's not synthesized by the traditional T RNA or DNA or messenger RNA, T RNA mechanism and its structure consists of five amino acids that are repeated trice and so I'm going to draw the structure of the molecule and I'll draw it kind of in a stylized fashion because I think that's actually useful for reflecting the confirmation of the molecule. So the molecule starts with a proline and we next continue with a valine and we next, it's a non-ribosomal polypeptide so we next have an, call it unnatural amino acid but it would be better to say non-proteinogenic or non-ribosomal amino acid and so the next one I'll label this as valine. The next one is ornithine. Ornithine is like lysine except instead of having a four carbon chain it has a three carbon chain, so one, two, three. The next amino acid is in the molecule is leucine and the final amino acid before we repeat ourselves is the unnatural enantiomer of phenylalanine so that's D-phenylalanine and so that's half the molecule and then the molecule repeats itself. So let me write leucine up here, then the molecule repeats itself and so now we're going to continue around with proline and the next amino acid is valine and then we come to ornithine once again and then we come to leucine. >> Do we need to draw up those [inaudible]? >> Just draw it. [Laughter] If you don't want to draw it out that's fine too. Do you have anything better to be doing right now? [Laughter] All right, as you can see there are a lot of different hydrogens in this molecule and one thing to keep in mind is there's actually some sense to all of this, in other words you'll look at a molecule like this and used say oh, well okay, alpha protons that's the proton that's directly next to the nitrogen and next to the carbonyl and you're going to say oh, wait that's next to an electron withdrawing group. It's tertiary and it's alpha to a carbonyl and so you'd say, oh, okay well, tertiary brings you down field. Next to a carbonyl shifts you down field. Next to an electron withdrawing group shifts you down field and you'll end up in the 4 to 5 parts per million range or you look at the beta proton say in valine that's one over and you'd say, oh, well, okay now that's beta to an electron withdrawing groups, so that's going to go down field a little bit. It's tertiary so that's going to go down field a little bit. So it's going to be a little down field of 2 parts per million or you'll look at the gamma protons, the ones on the methyl groups and you're going to say, oh, okay those are methyl groups that aren't really near to anything so those will be like.9 or maybe 1 ppm and so similarly we're going to have alpha, beta, gamma, delta for the ornithine and we'll have alpha, beta, gamma and delta for the leucine and alpha, beta and then all the phenyls which if you wanted to you could call them delta epsilon etcetera and then similarly for the proline alpha, beta, gamma and delta. So we start to make some is sense of this. Now one thing that's nice even if you're not an expert in this area, even if you don't do this stuff a lot what's nice is okay you can always sort of look up where things typically show up and so I will start with a little handout for you and basically what these data that I'm passing out are is really just what we've been intuited when I started to go through the valine there with an example. These are just typical chemical shifts of unstructured amino acids in water. By unstructured I mean not part of any sort of alpha helix or beta sheet and so pretty much just as I went through and said hey we can intuit that your alpha proton on your valine is going to be somewhere in the 4 to 5 parts per million region and your beta protons are going to be somewhere a little down field of 2 parts per million and your gamma protons are going to be somewhere around.9 parts per million. You can go ahead and look that up and you can do the same thing for leucine and so this basically provides you with good guidance for things you might already really, really know. I mean in other words you'll look say at ornithine and you'd say okay, well where should the delta protons at ornithine show up? Well you've got this ammonium group next to them. Nitrogen isn't the electron withdrawing so you'd say oh, about 3 parts per million but you could look and say okay, lysine, where does it say for the epsilon protons on lysine? And you'd say, oh, okay about 3 parts per million. My intuition is correct so this can be a nice help. The flip side gives you all twenty of the proteinogenic amino acids so you don't have to go ahead and know exactly what they are. All right, so we're going to use these to help us assign our resonances but of course ultimately because things will vary this compound has some structure to it. It happens to adopt a beta sheet structure. Things may not show up at exactly these positions plus every amino acid's neighbor will shift it around but you can look and say okay, where would I expect say the beta protons of phenylalanine to show up? And you can say well, it's a methylene. It's next to a benzene ring. It's beta to a nitrogen. You'd say oh, somewhere around 3 ppm or you could go ahead and say look, where would I see for phenylalanine? Oh, yeah, I'd see somewhere around 3 parts per million for the beta protons, all right. What I would like to do at this point is for us to look at the actual TOCSY spectrum of gramicidin S and so to answer your question, yes the structure is written out so if you're drawing really did look like a disaster then you have it here but then you'll have to keep flipping over and over again to keep labeling our resonances. All right so, what's funny? >> HOHAHA [laughter]. >> It's only good for one laugh. It never gets two out of people [laughter] and it's not even Christmastime. All right, so whenever I'm dealing with a heavily overlapping spectrum and I want to help my eyes out I like to slap a grid on the thing just to help me see things line up. You can also use a ruler but it's very, very nice and very gentle on your eyes to be able to say trace a cross peak over and then trace the cross peak right up over here, so I like to do that. Because TOCSY is like a super COSY you basically can trace an entire track off of TOCSY and get everything in a spin system. Now remember, a spin system isn't always the whole amino acid, so example in phenylalanine, the benzene ring is one spin system that's separate for all intents and purposes not coupled to the alpha proton, the beta proton, and the NH proton. I'll even draw in my NH, so this happens to be a spectrum in DMSO so this is in DMSO D 6 and this particular one happens to have a 78 millisecond spin lock, spin mixing time. Now one thing about molecules with NHs and OHs those generally exchange rapidly, so if I took a spectrum in D2O we would just see an HOD peak like we did in our hydroxy proline problem. We'd just see HOD but in DMSO D 6 the protons don't exchange so you're going to have NHs and so forth there. If you want to see your NHs in water you can actually do an experiment where you use 90 percent H2O and 10 percent D2O for locking so most of your protons, 90 percent of your protons stay as NHs and then you use water suppression because you're working with millimoles of compounds in hundred molar water, you know 50 molar H2O and 100 molar of protons. All right, so let us start and let's look at the anatomy of the spectrum. So the anatomy of our spectrum and I'll show you along this axis. Your alpha protons are over here. Your methyls are over here. Your NHs are over here. This is your phenyl group so I'll label it. We'll put all of our labels here so this is our phenyl group from the phenylalanine and let's see you've got some betas and gammas and deltas over here so. And so that kind of give us our starting anatomy. Our methyls are kind of at the.9 ppm range. Your alphas that are directly next to electron withdrawing groups are down here. Your NHs that are attached to nitrogen are over here. All right, what we're going to do now is use TOCSY to assign every resonance and I want to show you the power of the TOCSY technique and we'll just take a single track in the TOCSY, so I'll start off of this peak here that's a tight little doublet and I'll draw a line just to help my eye trace along and you'll look and you'll say, okay, so what sort of residue has an alpha proton and a couple of protons at about 3 parts per million? Is it the valine? What does the valine have in its spin system? >> Three protons. >> And what types of protons do we get in the valine? >> Oh, oh in terms of-- >> What resonance? What do you have in valine that you don't have in say ornithine or phenylalanine or proline? Methyl, so we would expect cross peaks somewhere up here. So it's not a valine. It's not a leucine. So we have alpha protons and one other sort of proton in that residue so what is that residue? And those protons are right around 3 parts per million. >> Isn't it proline? >> Phenylalanine because we just have two other protons, the two diastereotopic beta protons. So you trace your way up here and in this cluster of three which we could expand upon is your phe alpha and you trace your way up here and here are your two diastereotopic phe betas and you can kind of see the ABX pattern of one of the phe betas tenting into the other. So that basically assigns one of our residues. All right, let's go on to another one. Let me take this TOCSY track, so I'm going to label this guy as well. He's our phe NH so we're going to assign all the resonances here, so let me take this next TOCSY track. So what does this cross peak tell us? Methyl, so this is? >> Valine or leucine. >> Valine or leucine and what did I say about the gamma proton, the beta protons of valine? Methine typically it's beta to an electron withdrawing group so it's typically about 2, a little further down field than 2. This is so this is our leucine, so this is our phe NH. This is our leu NH, so I'll just trace that up to here on the diagonal so there's our leu NH. Our leu methyls are hiding right in this cluster here so that is our leu deltas and then our leu betas and gammas are lumped together over here. [ Silence ] Where's our valine hiding? >> The one that's below. >> Yeah, the one just below it. Look at that sneaky devil, sneaky devil. That valine NH is hiding right under the phenyl group and you wouldn't have known it except that darn phenyl is not part of a spin system with methyl group and here we see the cross peak for our valine gamma protons, the methyls and here's the cross peak for our valine beta proton and look at that. That valine beta proton has a nice splitting pattern because it's a hydrogen that's split by the methyls and also it's split by the methine. It actually ends up being a doublet of septets if you want a technical analysis for it. And hiding under here is our alpha proton. Oops, I meant to mark our-- I marked our leu betas and gammas. I marked our leu NH and so if I trace up here that guy is the leu alpha so I'm going to label him because we're going to victoriously assign every resonance here. So okay we've got our leu alpha. Now let's go on and we'll do our valine TOCSY track, so sneakily hiding under here is a val NH. Underneath this group here is our val alpha, right close to the phenylalanine alpha. Here's our val beta and underneath the methyl cluster a little bit off on the side if you trace your tracks is your val gammas. All right, so we've got our val. And this is our phenyl, so what do we left to trace out? So we've got one more. This is the whole NH region here so we've got one more NH but something's funny, something's funny about this. What's left for NH? >> Ornithine. >> Ornithine, proline doesn't have an NH. It's the one amino acid that doesn't have an NH, so this has to be, this has to be ornithine and yet you look at this guy and you say, wait a second? Okay, so we've got our alpha here. This has to be ornithine here. We've got our alpha. That's the alpha over here. We've got a bunch of stuff over here but remember what I said, the delta of ornithine is like the delta of lysine, it's like the epsilon of lysine. It's next to an ammonium group. It should be at about 3 parts per million. We don't see a track for it. Now we're doing a 78 millisecond spin lock time and remember I said the longer the spin lock time the more jumps you can make but of course there's the big caveat. If you go too long you've got relaxation. You're also putting a lot of power into the spectrometer for the spin lock mixing so you can't go too long or you're going to be turning your sample into cooked eggs. You're going to be heating it up with all the radio frequency radiation. So you have to go six hops to go from the NH of ornithine to the delta protons of ornithine and we're not quite going there in 78 milliseconds spin lock mixing time. So normally if you go there you see the same tracks repeated again and again. So for example, you get a TOCSY tract for the phenylalanine alphas where you can see here you get the on the phenylalanine you get the betas and you'll get the alpha proton here and then the NH over here but here we're not getting all of our cross peaks, so we're getting our ornithine betas and gammas. They're right under here but not your ornithine epsilon but look what happens now. If we haven't gone all the way through I can just pick a different TOCSY track. So instead of starting at the ornithine NH, I start at the ornithine alpha proton now look you get one more cross peak so you still have this cross peak here but now we get one more and there's our missing orn delta protons and so the orn delta if you trace it up, traces right underneath over here. So it's right over there. All right, we have only one residue left to assign at this point. All we have left to assign is our proline. This by the way is our ammonium so this is our NH 3 plus and so all I need to do is pick an unclaimed residue and work my way through. So we haven't claimed there guy yet, right? He kind of stands out and he's got to be something associated with the proline. He's too far up field to be a proline alpha proton so he's our proline delta proton, right? Alpha, beta, gamma, delta, so there we'll start with our proline delta proton and I'll just draw my TOCSY track. Proline of course doesn't have an NH so we have nothing out in the NH region and I can just trace all of my cross peaks. So we have my proline delta over here and then I can trace these guys up here so here's my proline alpha. It's lumped right under here, looks like it's a little bit down field so it's that guy right at the edge. There's our pro alpha. There's our pro delta right over there. I'll just, oops and then these guys over here are our proline betas and gammas. So I can just trace them right up and it's basically one of them is lumped under our water peak and then one of them is over here and then the last one is kind of right over here and so these guys are our pro beta and gamma. [ Silence ] And so the point in this is in very short order we've gone ahead and been able to get all of our resonance assignments for I don't even know how many different protons but bunch of different protons and it was a lot less painful and a lot more quick than trying to trace our way through a COSY and in a COSY, in that region with the betas and gammas where things overlapped heavily we would have been completely stumped. We would have traced our leucine methyls into the beta and gamma region and never been able to trace our way over to the leucine alpha or the leucine NH proton. We would have been lost. So that is very nice example of how TOCSY deals with overlap. All right the last experiment I wanted to present is ROESY. We've already presented NOESY. NOESY is a 2D NOE experiment. The big problem with NOESY is that you go from having positive NOEs to having negative NOEs as you go from small molecules to very big molecules. In that intermediate range molecules of say molecular weight of let say about 1000 to 1500 you often have zero NOEs and what ROESY is is NOES in the rotating frame. It's Rotating frame Overhauser Effect. So it's basically like NOESY but for intermediate weight. It's actually the same pulse sequence as a TOCSY. It uses a different level of power in the spin lock mixing and so it's good when you have molecules that have zero NOEs so I want to go ahead and show us the ROESY spectrum for gramicidin S and ROESY is particularly good for dealing with stereochemistry and conformational analysis just as we used NOEs to deal with stereochemistry in conformational analysis. In proximity you can use ROESY for the same thing. So I'll show you an example and I'll show you one little highlight. So here's our-- oh and I should give your next handout and actually I'll give us two handouts so I can finish us up here. So this is what I'm handing out right now is the ROESY spectrum of gramicidin S and I just want to show you what it's showing about the confirmation of the molecule and then what I'll do is just give us a little hint on the upcoming homeworks that will use ROESY and TOCSY. I'll grab a few more of these. If there aren't enough sweep them over. I made enough of these. All right I've actually drawn the molecule. I've drawn gramicidin S in a realistic confirmation. It's actually this extended confirmation and with what's cool about this extend beta strand confirmation is you can basically trace your way from residue to residue so each of your alpha protons are pointing, basically you're side chain is pointing out of the blackboard and back into your blackboard. The hydrogen here is pointing like this. The hydrogen here is pointing like this. The alpha hydrogen here is pointing like this while the valine side chain is pointing out and so what this ends up doing is it puts the inter-residue distance as very short and actually gives you a much further intra-residue NH alpha distance. So let me show you how this manifests itself in the ROESY spectrum of the molecule. So this region here and of course this region here is the cross peaks between the NHs and the alphas because we've got our NHs here in the 8 ppm range and the alphas in the 4 to 5 ppm range so we've just blown this up over here. This is actually from Nakamichi's [assumed spelling] book, Nakamichi blew this up. So let's go ahead and look at say this cross peak here. This is a cross peak between phenylalanine NH and leu alpha and you'll notice that that cross peak is very, very strong. Here's our phe NH, here's our leu alpha and then if you look at the other cross peak off of the NH it's much weaker. This is our, this one here is our lu NH, lu alpha. This is I'm sorry our phe alpha, phe NH to phe alpha. It's much weaker because they're not staring each other in the face. We see that same behavior over here. The one here is our lu NH to orn alpha and again these guys are staring each other in the face. Here's the lu N H. Here's the orn alpha and you'll notice the cross peak with the lu NH and the lu alpha is much weaker. Remember NOE cross peaks vary as distance to the inverse six, so if you have two hydrogens that are close to each other like two and a half angstroms you get a much stronger NOE than if you have hydrogens a little farther apart like three and a half angstroms. Remember that table I put up of relative intensities where it was like a ten-fold difference in intensity in NOEs. Finally here you have the orn NH to val alpha and so that's this one right over here, so you can see this sort of extended beta strand confirmation of the molecule. Okay, you're going to use this exact same type of analysis in your homework to assign all the residues in this molecule which forms a hydrogen bonded dimer and I want to give you a couple of little hints on it. One of the little hints is in assigning your resonances you'll be able to identify these methylenes, this methyl and methylene. You'll be able to use NOEs to walk your way over. You'll be able to use COSY and TOCSY to walk your way through the aromatic ring systems. You'll be able to look for hydrogens that are close to each other across the ring and see evidence of dimerization in your structure. Of course if you have two hydrogens that are symmetrical you won't see a cross peak between them because they're one resonance. Anyway, go ahead. Have fun with this. You will actually be able to apply these same skills to basically work your way through the spin systems. Do the TOCSY to get all you have your assignments and then do the ROESY to go ahead and figure out which hydrogens are close to each other. >> Can we see the ones in the middle? >> You can't see a proton with itself because if you have a hydrogen at 4 ppm and it's the same hydrogen at 4 ppm you can't get a cross peak so those two are symmetrical. All right, so that will be something you'll be doing I guess over the weekend. ------------------------------ac78f247e834--
B2 nh alpha spin beta molecule cosy Chem 203. Organic Spectroscopy. Lecture 23. Using TOCSY to Elucidate Spin Systems. ROESY 46 2 Cheng-Hong Liu posted on 2015/02/02 More Share Save Report Video vocabulary