Understanding NMR
Spectroscopy
James Keeler
University of Cambridge, Department of Chemistry
c James Keeler, 2002
1 What this course is about
This course is aimed at those who are already familiar with using NMR on a
day-to-day basis, but who wish to deepen their understanding of how NMR
experiments work and the theory behind them. It will be assumed that you are
familiar with the concepts of chemical shifts and couplings, and are used to
interpreting proton and 13C spectra. It will also be assumed that you have at
least come across simple two-dimensional spectra such as COSY and HMQC
and perhaps may have used such spectra in the course of your work. Similarly,
some familiarity with the nuclear Overhauser effect (NOE) will be assumed.
That NMR is a useful for chemists will be taken as self evident.
This course will always use the same approach. We will first start with
something familiar – such as multiplets we commonly see in proton NMR
spectra – and then go deeper into the explanation behind this, introducing
along the way new ideas and new concepts. In this way the new things that
we are learning are always rooted in the familiar, and we should always be
able to see why we are doing something.
In NMR there is no escape from the plain fact that to understand all but
the simplest experiments we need to use quantum mechanics. Luckily for us,
the quantum mechanics we need for NMR is really rather simple, and if we
are prepared to take it on trust, we will find that we can make quantum mechanical
calculations simply by applying a set of rules. Also, the quantum
mechanical tools we will use are quite intuitive and many of the calculations
can be imagined in a very physical way. So, although we will be using quantum
mechanical ideas, we will not be using any heavy-duty theory. It is not
necessary to have studied quantum mechanics at anything more than the most
elementary level.
Inevitably, we will have to use some mathematics in our description of
NMR. However, the level of mathematics we need is quite low and should not
present any problems for a science graduate. Occasionally we will use a few
ideas from calculus, but even then it is not essential to understand this in great
detail.
Course structure
The course is accompanied by a detailed set of handouts, which for convenience
is divided up into “chapters”. You will notice an inconsistency in the
style of these chapters; this comes about because they have been prepared (or
at least the early versions of them) over a number of years for a variety of
purposes. The notes are sufficiently complete that you should not need to take
many extra notes during the lectures.
Each chapter has associated with it some exercises which are intended to
illustrate the course material; unless you do the exercises you will not understand
the material. In addition, there will be some practical exercises which
1–2 What this course is about
involve mainly data processing on a PC. These exercises will give you a feel
for what you can do with NMR data and how what you see relates to the
theory you have studied. Quite a lot of the exercises will involve processing
experimental data.
Chapter 2 considers how we can understand the form of the NMR spectrum
in terms of the underlying nuclear spin energy levels. Although this
approach is more complex than the familiar “successive splitting” method for
constructing multiplets it does help us understand how to think about multiplets
in terms of “active” and “passive” spins. This approach also makes it
possible to understand the form of multiple quantum spectra, which will be
useful to us later on in the course. The chapter closes with a discussion of
strongly coupled spectra and how they can be analysed.
Chapter 3 introduces the vector model of NMR. This model has its limitations,
but it is very useful for understanding how pulses excite NMR signals.
We can also use the vector model to understand the basic, but very important,
NMR experiments such as pulse-acquire, inversion recovery and most
importantly the spin echo.
Chapter 4 is concerned with data processing. The signal we actually
record in an NMR experiment is a function of time, and we have to convert
this to the usual representation (intensity as a function of frequency) using
Fourier transformation. There are quite a lot of useful manipulations that we
can carry out on the data to enhance the sensitivity or resolution, depending
on what we require. These manipulations are described and their limitations
discussed.
Chapter 5 is concerned with how the spectrometer works. It is not necessary
to understand this is great detail, but it does help to have some basic
understanding of what is going on when we “shim the magnet” or “tune the
probe”. In this chapter we also introduce some important ideas about how the
NMR signal is turned into a digital form, and the consequences that this has.
Chapter 6 introduces the product operator formalism for analysing NMR
experiments. This approach is quantum mechanical, in contrast to the semiclassical
approach taken by the vector model. We will see that the formalism
is well adapted to describing pulsed NMR experiments, and that despite its
quantum mechanical rigour it retains a relatively intuitive approach. Using
product operators we can describe important phenomena such as the evolution
of couplings during spin echoes, coherence transfer and the generation of
multiple quantum coherences.
Chapter 7 puts the tools from Chapter 6 to immediate use in analysing
and understanding two-dimensional spectra. Such spectra have proved to be
enormously useful in structure determination, and are responsible for the explosive
growth of NMR over the past 20 years or so. We will concentrate on
the most important types of spectra, such as COSY and HMQC, analysing
these in some detail.
Chapter 8 considers the important topic of relaxation in NMR. We start
out by considering the effects of relaxation, concentrating in particular on
the very important nuclear Overhauser effect. We then go on to consider the
sources of relaxation and how it is related to molecular properties.
1–3
Chapter 9 does not form a part of the course, but is an optional advanced
topic. The chapter is concerned with the two methods used in multiple pulse
NMR to select a particular outcome in an NMR experiment: phase cycling
and field gradient pulses. An understanding of how these work is helpful in
getting to grips with the details of how experiments are actually run.
Texts
There are innumerable books written about NMR. Many of these avoid any
serious attempt to describe how the experiments work, but rather concentrate
on the interpretation of various kinds of spectra. An excellent example of
this kind of book is J. K. M. Sanders and B. K. Hunter Modern NMR
Spectroscopy (OUP).
There are also a number of texts which take a more theory-based approach,
at a number of different levels. Probably the best of the more elementary
books if P. J. Hore Nuclear Magnetic Resonance (OUP).
For a deeper understanding you can do no better that the recently published
M. H. Levitt Spin Dynamics (Wiley).
Acknowledgements
Chapters 2 to 5 have been prepared especially for this course. Chapters 6, 7
and 8 are modified from notes prepared for summer schools held in Mishima
and Sapporo (Japan) in 1998 and 1999; thanks are due to Professor F Inagaki
for the opportunity to present this material.
Chapter 9 was originally prepared (in a somewhat different form) for an
EMBO course held in Turin (Italy) in 1995. It has been modified subsequently
for the courses in Japan mentioned above and for another EMBO course held
in Lucca in 2000. Once again I am grateful to the organizers and sponsors of
these meetings for the opportunity to present this material.
Finally, I wish to express my thanks to Professor AJ Shaka and to the
Department of Chemistry, University of California, Irvine, for the invitation
to give this course. The University of Cambridge is acknowledged for a period
of study leave to enable me to come to UC Irvine.
James Keeler
University of Cambridge, Department of Chemistry
March 2002
James.Keeler@ch.cam.ac.uk
www-keeler.ch.cam.ac.uk