Chemical shift referencing your NMR spectra
There are various ways of referencing NMR spectra; however, they all
have potential problems with either systematic errors or
practicality. In general, there are three methods in wide
use:
- Adding an internal standard to the solution.
- Using an external standard which is typically a neat liquid.
- Using the chemical shift of the lock solvent as a reference for
other nuclei--basically a special case of the first method, where the
solvent is the internal standard. This is the default method in
both VnmrJ and in Bruker software.
The main drawbacks to using internal standards in general are that
their shifts change as they are diluted into different solvents, and
removing the standard may be a problem if you want to recover the
sample in pure form. Although we normally think of TMS as an
inert molecule, its 1H chemical shift moves more than 0.6 ppm as it is
added to common organic solvents, relative to neat TMS (e.g. benzene
+0.30 ppm, chloroform -0.14 ppm). Some specific primary chemical
shift standards are chemically reactive (such as
phosphoric acid) and either inconvenient (such as liquid ammonia) or
very dangerous (such as methylmercury) to handle. Phosphoric acid
and ammonia are also good examples of compounds whose chemical shifts
are so dependent on pH and concentration that they are useless as
dilute internal standards. In proton NMR of aqueous solutions,
DSS and TSP are both susceptible to changes in their shift at low
sample pH, when they become protonated. They are also capable of
intermolecular interactions with other solute molecules. For
example, they form host-guest complexes with cyclodextrins, which
changes the shift of the reference peak, and may disrupt other
host-guest equilibria in the sample.
Shift changes with dilution can be avoided by keeping the standard as a
neat liquid, unmixed with the sample to be referenced. However,
switching from an analyte solution to a separate NMR tube containing
the reference is frequently quite inaccurate because different samples
have different bulk magnetic susceptibilities; if this variation is not
corrected, it may introduce an error of up to several ppm.
External referencing of 19F and 31P to neat CFCl3 and 85% phosphoric
acid (this is the strength of the acid straight out of the reagent
bottle--the balance is water, and it must be used without further
dilution), respectively, suffer from this problem.
These solutions necessarily contain nothing deuterated to lock on, so
there is no way to compensate for the bulk susceptibility effects when
you switch samples and run the standard unlocked. The only
accurate way to use a neat reference solution is to put it in a
concentric insert in your NMR tube, the type used for determination of
paramagnetic susceptibilities by the Evans method. The
concentricity is important for good lineshape and best
accuracy--inserting e.g. a sealed melting point
capillary into the sample, with nothing to hold it in the center of the
outer tube, frequently will not give very good resolution. (As an
aside, the
Evans method would not work correctly either if the two solutions were
run in separate NMR tubes at different times.)
Some time ago, the concept of expressing NMR frequencies in Xi (as in
the Greek capital letter) units was introduced in multinuclear
NMR. This is the calculated frequency of a signal where the 1H
frequency of TMS is exactly 100 MHz. These numbers are calculated
by measuring the exact frequency of the peak of interest, and the exact
frequency of the 1H TMS peak, on the same sample at the same time with
the spectrometer locked; then determining the ratio of the frequencies,
and multiplying by 100 million. To translate that number into the
expected frequency of that peak on your spectrometer, you find your 1H
TMS frequency, divide by 100 million, and multiply the reported Xi by
that number. NMR frequencies can be measured with very high
accuracy, better than 0.1 Hz; the ratios of these numbers are equally
precise, and they are instrument independent. In this
way, the chemical shift scales of all nuclei can be tied together
with ratios. If we have one careful measurement of the ratio of the 1H
TMS frequency to the 31P frequency of phosphoric acid in a coaxial
insert, or the 15N frequency of liquid ammonia, and we know our 1H TMS
frequency, then we don't need the actual multinuclear external standard
to produce correctly referenced multinuclear spectra. The IUPAC
has adopted this method of chemical shift referencing and published
tables of Xi values for the NMR active isotopes. Varian's
implementation of the IUPAC values is in the file
/vnmr/nuctabref. For some nuclei, more than one chemical shift
reference has been used over time. In those cases, the one
used by VnmrJ will be the first uncommented line for a given
nucleus. For example, nitrogen chemical shifts have been reported
relative to neat liquid ammonia, neat nitromethane, and
tetramethylammonium iodide in DMSO. Biological NMR spectroscopists
report nitrogen shifts on the ammonia scale, while organic chemists
tend to use the nitromethane scale. These scales differ by 380.2
ppm. Although they are less different, bio-NMR spectroscopists report
13C shifts relative to DSS in D2O, which is offset from the 1% TMS in
CDCl3 scale used by organic chemists by a few hundredths of a ppm.
A ratio scale can be converted to an absolute scale if we know the
frequency of any one point on the scale in absolute numbers. In
practice, what both Varian and Bruker do is to use the known absolute
deuterium lock frequency, rather than the 1H TMS frequency, as the
basis for all multinuclear chemical shift calibrations. This has
the advantage that you do not have to have TMS present in every sample
in order to establish chemical shifts. Both vendors' software can
be optionally configured to check for TMS in the spectrum and set the
shift to exactly zero if the peak is found, or make no changes if it is
not. This system can work extremely well, although there are
various potential problems to be aware of.
- You must have the sample locked. This method doesn't work at all
if you have no deuterated solvent present, or run the spectrum
unlocked, or incorrectly identify the name of the solvent.
- For solvents that have more than one peak in the proton/deuterium
spectrum, the peak you are actually locked on must correspond to the
peak the software is looking for. Methanol, toluene, and THF are common
solvents that have multiple peaks.
- The chemical shift of the solvent must be known and its chemical
shift defined in the software. The solvents known to VnmrJ are in
the file /vnmr/solvents (the first number after the solvent name is the
assumed chemical shift of the lock.)
- Different sources or software packages may use slightly different
values for solvent shifts. It is a good idea to be consistent
about the way you set solvent shifts, whether it is according to VnmrJ,
or MestReNova, or the reference list from Cambridge Isotope Labs.
- The lock solvent chemical shifts are a good approximation as long
as your sample is a sufficiently dilute solution to be a good
approximation of pure solvent. Highly concentrated solutions may
pose problems. Also, mixing two deuterated solvents will likely
perturb the shifts of both solvents and render the shifts
inaccurate. Unless you absolutely have to use a mixed solvent in
order to get adequate solubility, or you are trying to reproduce
published shifts reported in a mixed solvent, it is best not to. Mixed
solvent solutions also can cause problems with autolocking and with
gradient shimming.
- D2O is particularly problematic because its chemical shift is
very temperature dependent--it moves upfield 11 parts per billion per
degree as the temperature increases--and also depends on pH.
Varian assigns the value of 4.67 ppm as the 1H shift of D2O. This
is true only at a single temperature (apparently an above ambient
temperature), which may not be the temperature of your sample. If you
use DSS to circumvent these problems, note that DSS has a pH dependent
shift, and can associate with other solute molecules, as described
above.
- If you have silicone grease in your sample (and who doesn't), you
will have a 1H peak at 0.08 ppm, which can be mistaken for the TMS peak
if there isn't any TMS, but the software is trying to zero on
TMS. If this happens, all your peaks get shifted upfield by 0.08
ppm. Checking for a peak at zero if you know you didn't add TMS
to the sample, or an error in the shift of the solvent peak, may help
you catch this.
- If you are in doubt about whether the default referencing has
been applied (e.g. for a nucleus where you are not very familiar with
the expected chemical shifts), go to the Process -> Default tab, and
under Reference, click the button that says By Solvent. VnmrJ can also
reference the indirect dimension correctly in a 2D or 3D
experiment. For 2D experiments, there are separate buttons on the
Process -> Default tab for referencing f2 (direct) and f1 (indirect)
shifts by solvent. Redisplay the 2D spectrum after clicking these
buttons.
My personal preference is to use the solvent based referencing scheme
for all nuclei, unless I know the prerequisites for having it work are
not met, such as running unlocked, or with a nonstandard solvent.
Dave 7/23/09