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  • >> 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--

>> So when we were talking about coupling constants,

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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)

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    Cheng-Hong Liu 發佈於 2021 年 01 月 14 日
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