字幕列表 影片播放 列印英文字幕 >> So when we were talking about coupling constants, I said sometimes there are some really big differences between coupling constants, distinct differences between coupling constant so like an alkanes, if you have a cis coupling, your J3 H-H is about 10 Hertz, if you have a trans coupling your J3 H-H that's your three bond coupling or your vicinal coupling is about 17 Hertz and by the way I will again caution you to make sure you understand the difference between coupling through a double bond versus coupling between double bonds so a lot of people particularly when they are starting out confuse stereochemistry with confirmation. You can rotate about single bond so even if you have a bond between two single bonds that might be S-cis or S-trans that's always a dynamic equilibrium. It may be heavily weighted toward one way, but that's not stereochemistry that's confirmation and that by mind you has a different Karplus curve then the Karplus curve for an SP2-SP2 carbon pair that's connecting two hydrogens. So anyway this is specifically not on here but let's now talk about cyclohexane which is what I'm going to choose for today's, today's lecture and just remind us of some of the key features I pointed out, previously we talked about the Karplus curve for SP3-SP3 systems and we said that there are some very distinct relationships that are, that in cyclohexane, so 180 degrees gives you a big coupling constant, a 60 degree relationship gives you a small coupling constant. So our axial-axial coupling has a 180 degree dihydro relationship, those of you who saw the previous sophomore class that was just filing out got to see Hanna talking about Newman projections and if you're Newman project you have a 180 degree dihydro angle and typically you have about 8 to 10 Hertz for an axial-axial coupling. If you have an axial equatorial coupling, these are of course all three bond couplings. We're in equatorial-equatorial coupling, you have a 60 degree dihydro-angle and you remember the Karplus curve that I drew out before and so that's about 2 to 3 Hertz for each of those. So what I'm going to do right now is pass out a or, or mention a very real example that just came up in my lab and I thought it would make a cool, cool example for spect and it was a stereochemical problem associated with the conjugate addition to a, an alpha, beta and saturated nitro compound. So we were working with nitrocyclohexene, the nitrocyclohexene is electrophilic at the beta position and we were doing an addition of aniline, I'll write that as pH, NH2 to give the addition product. [ silence ] and so the issue here was whether we have the trans product [ silence ] or the cis product [ silence ] and so of these two stereo-isomers what do we call the relationship between these stereo isomers? Diastereomer, so of these two diastereomers each of them of course is formed as the rasimic and that doesn't matter because you can't tell one enantiomer from another by NMR, the spectrum of a racemic mixture is identical to the spectrum of either in individual enantiomer unless you have some sort of chiral solvent or unless I prepare a chiral derivative. So the only way I could distinguish these two apart would be say to make an amid the two enantiomers apart would be to make an amid where I had a chiral acid brought in to make an amid or to use something like a chiral shift reagent or chiral solvating agent. So the big question is which of these two is formed, the cis, the cis or the trans and I want to pass out the spectrum, we will take a lot and analyze it. [ silence ] And I have a few extras here, and some anyone else? One more back here, great. [ silence ] . Alright, great, so we have here the NMR spectrum and chloroform solution and what I've done here is I've blown up this region, the midfield region so we call this region the downfield region, this real region, the upfield region and I'll call this the midfield region. So our molecule of course is night has a fennel group in it and so I think it's pretty obvious that our fennel group is over here. You might notice for example if you look at the fennel group that we have something that looks like a doublet or an apparent doublet that corresponds to the ortho protons. There may be some metacoupling going on there, we're not going to be talking in any great detail about this, but I just want you to get in the habit of always reading your spectrum so that corresponds to the ortho. We see something that looks like a triplet, that's the same integral, if you notice the height in the integral from here to here is identical from the height from here to here so that triplet or apparent triplet corresponds to the meta protons, there are two of those and then we see something that looks like a triplet over here and again it's either triplet or an apparent triplet or there's some small additional coupling, let's say HM and that corresponds to the power of proton. I don't know if you can see on here, but you certainly can see on yours, do you notice where the ortho-proton and the meta-proton and the, and the para-proton show up? What's their chemical shift roughly? 6.6, 6.7 I said aromatic are typically 7 to 8. Do you know why they're little upfield? Nitrogen donation, so the electrons pushing in from resonance off of the nitrogen. By resonance, we get extra electron density at the ortho-position and the para-position and so that ring is shifted a little bit upfield which is kind of cool. If I made an amid out of that nitrogen which would pull electron density out, these guys would scoot over a little more downfield and here this little guy over here this is your core form [inaudible]. Alright, all of this is all of the other cyclohexyl stuff [ silence ] that are not directly involved and then we have three peaks in the midfield region. Remember right now we don't know stereochemistry and we don't yet know what's what. Why do we have three peaks? The NH, so we have these two protons and the NH. Something very interesting happened with this sample and this wasn't anything that I'd planned on, it was simply the day, a day later I went to rerun the sample, same sample and the midfield region looked a little bit different. This is your day old, day old sample, this is the freshly prepared sample. What's going on there? [ silence ] . So we still see it, so James said the nitrogen is swapped with deuterium so we still see it, but now it's broad. What does that tell us? Maybe moist. If it were very, very wet, you see this peak over here, so this is and the sample was nicely sealed so this little peak here at 1.6 is H2O, that's about where you see at 1.6, 1.56 that's very typical for H2O on chloroform, so we don't have a lot of water in there, probably about 10 millimolar, 20 millimolar water and we have lots and lots of sample and what else did I tell you about chloroform? Can generate HCl and a little bit, even a little bit that forms is going to catalyze the acceleration, the exchange of NH's between molecules or between molecules and water so even if you form just a little bit 1 percent for example of I guess would be DCL but the majority of course if it's one percent of your, you know of your molecule, one molar percent majority is still HCl, but what's happening is now your NH is instead of saying attached to the same molecule are getting swapped between molecules and as a result in this case it's also getting swapped with water, but as a result if that proton doesn't stick around for tens of milliseconds or hundreds of milliseconds you can't see the spin as to whether it's been up or spin down, so we lose coupling, it becomes a singlet, in this case a broad singlet. Now let's look at these patterns here in the unexchanged samples, so these are all the midfield. So which ones the, the NH over here? 3.4 ish, the doublet, is the NH and so the other two and we'll talk more about this in a moment, but the other two, one of them changes a little bit in pattern visibly. Alright let's, let's talk now about what we call these patterns. So what do we call these patterns, we saw it last time. It's a triplet of doublets, you have two big coupling constants and one small coupling constant. What do we call this pattern here? A quartet of doublet, so you're having roughly 1:3:3:1 ratio for little doublets and if you wanted to be fussy about it you could say well you know my quartet isn't quite perfect, I can see these two aren't quite the same or they're ones litter fatter than the other you know because all for coupling constants may not be exactly the same, but they're the same within a Hertz or half a Hertz basically that within the line within the limit of digital resolution. So if you didn't like to analyze it is a QD you could call it an apparent QD, I'm fine with either. I think either of these accurately reflects what you see and here if you said you know I kind of sort of see a little humpy thing over here and over there, you could call it an apparent so I'll write or apparent TD, I'm happy with either analysis on this. Alright, so and you'll notice this peak simplifies the quartet of doublets simplifies which makes sense because that must've been the proton that was coupled to the NH group because we lose that coupling so that quartet of doublet now has become a TD or an apparent TD. Well it's not deuterium, remember even though you're getting a minuscule amount of DCL, let me put it in numbers. This sample is 50 millimolar roughly, we have may be generated 0.5 millimolar DCL, but that DCL is enough to catalyze the exchange so now this NH isn't sticking around on this molecule every millisecond this NH is bumping into another molecule and trading partners or every millisecond this molecule is bumping into NH a little bit of the H2O in the sample and trading partners. Typically when I prepare sample like this I pass the solvent through flame or furnace dried alumina to remove traces of water and DCL first if I want a nice spectrum or DMSO-D6 is another good solvent because if hydrogen bonds nicely and typically keeps your OHs in place by stabilizing them, so carboxylic acids that are hard to see in chloroform often show up well in DMSL. Question? >> [inaudible] >> And the water, so the water could help the exchange, but apparently not enough that it actually you know that proton actually does stay in place very nicely and it's just when you get some acid in the sample. >> Yes so I was saying that the double, the double, the NH doubling [inaudible]. >> A singlet so we would call this a broad singlet, BRS >> But then the QD [inaudible]. >> So okay, great question. The QD is becoming a TD and remember how we teetered on the edge here between being a triplet of doublets and you can kind of see a little bit of humpy stuff, all the 3 J's aren't exactly alike, they're all different sorts of protons with their own specific dihedrals coupling to it. So there are some differences and so depending on the shimming of the instrument, one day one time it looks like a TD and the other time this looks like a DDD with two very, very similar coupling constants so we can just at this point see eight lines here and so at this point just due to chance of the shimming, we're able to resolve the two coupling constants that differ by about a Hertz so becomes a DDD that's, this is purely, purely coincident. If I had this with slightly less good shimming it would have worked exactly like that. Alright, what I want us to do now that we thought about this a little bit is to extract the stereochemistry from here. So we by figuring already actually happen to know then that this proton here corresponds to this one, this one here corresponds to that one, but even if we didn't, we'd be able to figure, even if we didn't have this spectrum, you'd be able to figure that out by the amount of splitting that you see. Okay at this point I want us to focus on these lines, I want us to extract our coupling constants and I'm going to show you how I, how I handle my own data, I'd make things bigger on the back so this is a peak printout, I'm a big fan, you get this from a second a separate command on the spectrometer, I'm a big fan of getting these peak printouts because in addition to giving you the peak frequency of each line in PPM, it happens to give it to you in Hertz which of course you can calculate just by multiplying the spectrometer frequency, but the other thing that's really useful is it also gives you the peak height, so that if you have little stray peaks or if you have either an impurity or non first-order coupling in there you can pick out your main peaks. Here everything happens to be very, very straightforward, so that first multiplet the one that's the triplet of doublets has six lines to it and so I'm just drawing a line with my pen, the quartet of doublets has eight lines to it and the doublet of doublets has two lines, the double has two lines to it. Alright, so remember our analysis of a triplet of doublets, we split with a big J into a triplet in other words we have two of the same big J and then we split each of those lines further into a doublet and so we get this one to two to one pattern where the lines on the outside are relative hide half the lines on the inside and if I called my lines, if I called my lines 1, 2, 3, 4, 5, 6 then the distance of the big coupling is 1 to 3, it's 2 to 4, it's 3 to 5, it's 4 to 6. [ silence ] . What did I say? 1 to 3, 2 to 4, 3 to 5, 4 to 6 is our big J and 1 to 2, 3 to 4 and 5 to 6 is our small J and you can see that here. So we're dealing with real data now. What I showed you before was simulated data all those lines were exactly the same distance apart because it was fake data because it was a simulation, so now to get the most accurate value of our J's remember you've got digital resolution, you've got the fact that your two coupling constants may not be exactly identical, but we can't extract them separately because we're not seeing separate lines turns out on that later spectrum where you did see the pattern resolve into a DDD, I was able to extract them, you'll get practice, we got practice with a DDD, remember 1 to 2 and 7 to 8 is your small J and 6 to, 6 to 8 is your medium J and then 1 to 8 minus big J, medium J and small J is your big J for DDD, but here all we can do is extract it and analyze what we see, which is one big J and one little J. So okay to get the most meaningful data out of here I'm going to take all of those numbers an average them, so get a sharper pen here because it's a lot of writing to do here. So if I take these and I've jotted it down normally you could do this with a calculator, so I've jotted it down here the 1 to 3 is 12.282, the 2 to 4 is, I'm sorry it's 10.282, the 2 to 4 is 10.253, the 3 to 5 is 11.154 and the 4 to 6 is 11.280 and those are our big J values so what I'm going to do is average them of all of that, of all the 1 to 3, 2 to 4, 3 to 5 and 4 to 6 and I got the average is 10.7 Hertz. And now I'd take 1 to 2, 3 to 4 and so forth and the average of those is, well let me get the numbers 4.065, 4.036, 4.162, so the average of those is 4.1 Hertz. [ silence ] . Alright, so if we wanted to report this peak the way I would report this peak to tabulate it to give us the short story is 4.38, I'd call it a TD or an apparent TD, maybe because I'm seeing that there is some deviation here I might call an apparent TD. J equals oops, put a comma there, J equals 10.7 and 4.1 Hertz and I didn't go do the integral here but if I did the integral I mean I did it but not now, it would be one hydrogen. [ silence ] . Thoughts or questions at this point? >> [inaudible]. >> I'll take the, I take the average of it. I want to show you something now I like to do. I like to take that peak printout and throw it into a spreadsheet. You will find a most of the problems that I have assigned I actually have a digital version that you can highlight with your cursor, paste into Excel or whatever spreadsheet program you use this one happened to have been done awhile ago and so I didn't, a didn't do that but it's very easy if you can slap the data in a spreadsheet. Even if you can't I'm a huge fan of this, so somebody help me out here because if I make a mistake normally I proofread, I'll just do 11.87, 0.921, and you'll see how quick and easy this is, 11.83, 1183.63, 0.680, 11.77, 1177.774. Am I doing that right? 1177.1173, by the way number pads are also extremely useful on this 1167.305 for data entry but again I'm a big fan of pasting stuff in and you'd definitely want to check your data because the literature is just full of crappy errors in data and you do not want to be contributing garbage to the literature or to put it more in concrete terms you don't want your committee going in handing you back your second, your report with a nonpassing redo on because you've contributed garbage. Okay so I think I have all of our numbers there, okay so this is a quartet of doublets so it's going to be 1 minus 4, 1 minus 3 and it's also going to be 2 minus 4, 3 minus 5, 4 minus 6, 5 minus 7 and 6 minus 8, so I can get all those values and I can just take the average. [ silence ] . And I get 10.3 Hertz, so that's our big J and our small J is 1 minus 2, whoop and it is 3 minus 4 and it is 4 minus 6, 4 minus, 3 minus 4, 5 minus 6 and 7 minus 8 and I can again just take my average I guess haven't pasted it all the way down and obvious what the average is there but. Alright so the average there is 4.1 Hertz. So I can go ahead and transcribe my analysis over and of course normally I would be sitting at my desk probably with the spectrum in front of me or my group members would be sitting, sitting at their desk. So the next one we can describe as a 3.90 QD or apparent QD if you prefer 10.3 since it really did look like that analysis was completely on, I'd call it 10.3, 4., oops J equals 10.3, 4.2 Hertz, 1H and usually if I'm being good particularly with my computer I will separate numbers from units so I will separate put a space in here, put a space in there because you separate numbers from units and the space here, the space here and the last one I didn't do but it's our doublet, it's 3.41 and it's a D that's just the difference between these two lines which happens to be 9.5 Hertz and that ends up to integrating to one hydrogen. Alright thoughts or questions? >> [ Inaudible question ] >> The nitro next, what's that? [ Inaudible question ] >> Between the two ones. Let's, let's find out. So now we've extracted our data, now it's time for us to analyze our data and figure out the stereochemistry of the molecule and also to think if there are any, any conformational issues. [ silence ] . So generally when you have a problem where there are two possible answers, the best way to approach it is to go ahead and to try one answer see how it fits, try the other answer, see how it fits and see if you can distinguish them apart. So I'm going to go ahead and draw a cyclohexane ring and let's start with the trend stereoisomer and if we have the trend stereoisomer, I'd assume that the favorable confirmer would have the two substituents in the equatorial position. [ silence ] . Now I wouldn't have known this am priori in terms of the confirmation of the amino group, but that NH coupling was pretty big that was a doublet with 7, with 9.5 Hertz, that's consistent with an antiperiplanar confirmation. Remember that's not stereochemistry, that's confirmation, but I can be pretty darn sure that it's realistic to draw this like this. So thing that I know right now is this is our doublet with J equals 9.5. Alright, if we have this molecule, this proton here how many big couplings would we expect to it and how many small couplings would we expect? >> Two. >> Two antiperiplanar couplings, so we have this axial proton giving an axial-axial coupling to this one, and an axial-axial coupling to this one and so okay and one axial-equatorial, so we would expect it to be something akin to a triplet of doublets with the J of the triplet, the big J of about 10 and a little J of about 3 and so what we see here is actually a TD or apparent TD with J equals 10.7 and 4.1 Hertz, so it's the data that we extracted and that seems, seems to so far be pretty reasonable. Alright, what would we expect for this proton? Somebody else. Three axial couplings, so we would expect and again we wouldn't am priori know whether I'd expect a big coupling or a smaller coupling or no coupling at all to this NH, depends on the confirmation. If you draw the phenylin it actually makes a hell of a lot of sense that it sticks out like this, ah you know in another words that it really does push it anti, antiperiplanar but am priori I might not know what to expect, but it expected least a big coupling from this guy to this guy axial-axial and at least a big coupling from this guy to this guy and we know from the J of the NH that at least in the fresh spectrum and fresh sample we have big J there so what other couplings would we expect to it? One axial-equatorial. So this one here we would expect to see as something like a QD or an apparent QD [ silence ] and we'd expect to have three big couplings and what we see is J equals 10.3, 4.2 Hertz. Now coupling should be mutual and coupling is mutual, but as I said you're lying with digital resolution each are about a Hertz, digital resolution's actually a few tenths of a Hertz lying with is probably about, about 1.2 Hertz, but within the limits of the digital resolution and more importantly the lying with we're not getting a separate splitting here. Did oh over here we see 10.7 which within the limits of experiment is the same here, in fact you could see that we were kind of teetering on the edge between that QD and a D-D-D type of or seeing some of our additional splittings because you could see all those spacings weren't equal, but we couldn't resolve it any better on this. So we see a QD or an apparent QD with 10.3 and 4.2 and this is what I'd report and it's consistent with these data. But now we also need to think this is super, super important because think about this, you start on a total synthesis of a natural product, you do a key step that gives you stereochemistry early on in the synthesis and you make a wrong conclusion and now twenty steps later you finally get your natural product except it doesn't match the public spectrum and you're in trouble and you're ready to graduate and you find out that your, your synthesis of isn't going to be titled total synthesis of hard complex molecule, but rather total synthesis of epi-hard complex molecule and that's not nearly as good, so this is really, really important to get this right. Okay, let's take a lot here, so imagine for a moment that instead of having the molecule as the trans stereoisomer, we had the molecule as the cis-stereoisomer and I don't know if the nitro groups going to want to be axial or if the nitro groups going to want to be equatorial or from going to expect some conformational mixture rapidly equilibrating, but let's start with the premise may be, may be it would be axial and let's think things through, I think it's pretty reasonable to assume that the trends is all equi, is both equatorial, diequitorial because diaxial would be the ring flip and would be two big substituents axial, but here we have a nitro group and an aniline group, but they're both kind of big [ silence ] . So what would we expect to, for this proton? Alpha-2 and a nitro group, alpha-2 and axial nitro group. Three equatorial couplings, so what would you, what would you expect that to be. Like a quartet with what sort of J? Something like 3 Hertz. Q, I'll say it might be an apparent Q, something that looks like a Q, J equals I'll say approximately go little squigglies, 3 Hertz, so that would be our prediction for this molecule. [ Inaudible ] >> Three equatorial, oh, axial, equatorial-equatorial about 3 Hertz, equatorial-axial about 3 Hertz, equatorial-axial about 3 Hertz. Now here's the cool thing, let's suppose you couldn't even resolve the multiplet, let's suppose the multiplet was a little broad and misshapen, you could look at the multiplet and say, so let's say for a moment that that multiplet looked, now let me give it a lot more structure to add. Let me, let's suppose our multiplet looks like that, not pretty, like it's a snake that'd swallowed an elephant to something. Alright, you could go ahead and say I can't get a peak printout on this thing, but I can measure this distance with my cursor. If that distance looks like it's about 12 Hertz, that sure as heck is not consistent with this one here because this one even if you couldn't resolve it, even if you couldn't exactly [ silence ] pick it out what would that distance be about? About 25 Hertz because we'd expected to be 10 or so plus 10 or so plus 3 or 4 or so, so in other words we're using the number 10 Hertz which was just a sort of the number I wrote on the blackboard or 8 Hertz or 9 Hertz, I would expect it to be at least 10 plus 10 plus 3, two big couplings of about 10 Hertz each and one little coupling of about 3 Hertz each, so that molecule even if it didn't give me its coupling constants precisely would scream at me that it was consistent with this and not consistent with this. Now what would we expect to see for this proton here? Let's assume that we continue to have coupling to this NH and it's about 10 Hertz, what would we expect to see here? [ Inaudible ] >> Two, so two diaxial couplings or. Alright, good so we would expect to see it as how would we describe that pattern? [ inaudible ] . A triplet of triplets [ silence ] or TT or something that looked a heck of a lot like it. Now I don't like calling this an axial coupling because that's special, I mean it's it happens that we happen to have it be big here, but it's not really axial on here, but you think of it because it's not on a ring, it's not axial on the ring, but we see it's big. Anyway the point is you would have one big coupling on the cyclohexene ring, one coupling to the NH that in this case we happen to know is about the same size and then two small coupling and so our pattern would look like 1, 2, 1, 2, 4, 2, 1, 2, 1. >> [ Inaudible ] >> They, they couldn't, so great question. So the question for example is why do they not split differently and the answer is they could split different or the same if the dihedryl angle is similar then you will see either the same or very close to the same, if the dihedryl angle is different you'll see different. It may be and we saw that how this was teetering with the spectrum where coupling constants that were the same within about a Hertz weren't quite resolving apart, 11 and 10 Hertz, 9.5 and 10.3 so it might be that this pattern instead of being a Q could be a TD or a DT or a D-D-D with three small Js. For example it could be a D-D-D with 4-3-2 and that would be consistent with this or a TD with 3 and 2 or DT with 2 and 3 or 4 or 3and that would be consistent, so three small Js. Alright, I want to play with this idea for a moment longer and ask the question what would happen if my assumption about the aniline group being equatorial was wrong or was incomplete and so I'll do a ring flip and imagine for a moment that my aniline group is axial and my nitro group is equatorial [ silence ] and so if we had this conformer so these are both cis, we have two different conformers here that we're considering. [ silence ] So let's take our proton alpha to the nitro group. What would we expect for this proton now in this conformer of this cis-diastereomer? [ Inaudible ] >> One axial so it's this one to this one and two equatorial partners so one axial-axial coupling and two axial-equatorial coupling, so how would we describe this proton here. [ Inaudible ] >> A doublet of triplets, DT or apparent DT and what would we expect their J's to be? [ silence ] . First name for the coupling constant, for the multiplet is doublet so that's the big split, 10, something yes 3,4 something, something like that. So we would expect it to split with the big J and then split into a triplet with roughly this small J and so the pattern you'd see is something like 1-2-1, 1-2-1 with this distance here being 3, 3, 3, 3, 10. And this guy here and let's assume again that we still have a big coupling to the aniline, so the one that's alpha to the nitrogen here what do we expect for him. >> [ Inaudible ] >> Two large so I'm assuming we're large to the nitrogen that's kind of a wild card and then Wurtz coupling partners on the right. The axial so this is axial-equatorial, this is, is equatorial-equatorial, this one. [ Inaudible ] >> So what are we? >> Two axial-axials, two equatorial-equatorial. >> We have, I'm assuming we're big J to the nitrogen. Let's assume, let's just assume because we happen to see that that NH was split so I'm assuming that's a big J. What are all of our other J's? All small. So, so this one we would expect to see as a DT, as a DQ or apparent DQ depending on how it is and this one we would expect to see the big J3 and the small the big J10 and the small J3. Alright, last thing I want to do [ silence ] alright let's call this cis-conf1 and this cis-conf2. Now imagine that we had an equilibrium which you may very well a conformational equilibrium they're two big substituents between cis-conf1and cis-conformer2 and that equilibrium is going to be rapid because ring flip on a cyclohexene is rapid and I just want us to think now about one of these protons. Let's just talk about what we would see for the proton that's alpha to the nitro group which I'm going to call H sub A and what I want us to think about is it's coupling specifically with proton B, proton C and proton D. We'll call B and C the ones that are ones that are on the methylene group and the back D the one that's on the methylene group on the front and so B is axial, C is equatorial here and this is D and what I want us to do is think about what we would observe if we had a dynamic equilibrium between conformer-1 and conformer-2, what would we expect? So if we look at JAB and conformer number 1, it's about 3 Hertz because it is an equatorial-equatorial coupling. If we look at JAC, it's also about 3 Hertz because it is an equatorial-axial coupling and if we look at JAD it also about 3 Hertz and that's why we say that proton was a quartet. In conformer number 2 if we look at it, JAB now is very different it's about 10 Hertz because AB is axial-axial, AC is axial-equatorial so it's still about 3 Hertz, AD is axial-equatorial so it's about 3 Hertz. So now if we are somewhere in the middle here, not all conformer-1, not all conformer-2 we would now expect to see one coupling constant that somewhere between 3 and 10 Hertz and two coupling constants that are both about 3 Hertz so we would now expect to see this as DT or an apparent DT or something that showed two big, one big coupling and two small couplings, in other words a J big of 3 to 10 Hertz if it were right in the middle we'd say about 7 Hertz so that might be my first guess and J small of about 3 Hertz. [ silence ] . So regardless of whether we had this cis as one conformer, the cis as the other conformer or the cis is a dynamic equilibrium in which both conformers are present are observed data of a triplet of doublets with 10.7 and 4.1 Hertz strongly matches the trans and does not match the cis, so that gives us a stereochemistry. Alright, we will pick up next time talking about other aspects of structure in NMR and specifically I guess we'll talk about coupling involved in other nuclei. ------------------------------9d5d74c52e0a--
B2 中高級 化學203.有機光譜學。第十四講.自旋-自旋耦合 (Chem 203. Organic Spectroscopy. Lecture 14. Spin-Spin Coupling) 36 3 Cheng-Hong Liu 發佈於 2021 年 01 月 14 日 更多分享 分享 收藏 回報 影片單字