Assignment 4
NMR Guided Reading
February 13, 2000
Overview:
This week we are going to start our investigation of the physics behind the
NMR experiment. This will include a thorough introduction to the rotating
frame, vector diagrams, the effects of on-resonance pulses (radio frequency
fields), quadrature detection, and phase cycling. That should be enough
for the week probably.
You will probably have heard of almost all (if not all) of these topics
before and may be somewhat familiar with the concepts. Understanding of
these ideas is crucial for our foray into 2D NMR spectra later on the
term.
Start the preparation this week by carefully studying sections 4.1 through
4.3 in Derome's book. Below are several questions/problems to help you study
this material. Answer the questions and turn them in on Wednesday.
We will continue on Thursday, based upon that information. After a
discussion of any difficulties and an introduction to the necessary
parameters/controls of the spectrometer, you will perform two experiments on
Thursday. The first of those is Experiment 2.8 described in 150 and
More . . .; the second involves modification of the Phase cycling program
for the simple 1H experiment and observing the effects on the observed
FID/spectrum. I will provide you with a writeup for that experiment
sometime this week.
Questions:
These are the questions to ask yourself while reading Derome (and then answer
and turn in). The relevant pages of Hornak's NMR
web page, if you want a second opinion on the material, are here: Spin
and Spin Physics
- Magnetically active nuclei (with I=1/2) can be oriented in one of two
directions when placed in a magnetic field. What are those two
orientations and which one is preferred?
- The interaction between the magnetic moment vector (m)
and the static magnetic field B0 results in precession of the
magnetic moment vector around the static field vector. Given that any
one nuclear magnet can have only one of two possible orientations, explain
in your own words why Figure 4.2 shows a cone of magnetic moments.
- Pay particularly close attention to Figure 4.3. Explain how both
diagrams are an accurate representation of the following equation.
F(y) = y cos (wt)
- In the rotating frame half of Figure 4.4, one of the radio frequency
vectors is neglected. On our spectrometer, what frequency would this
vector have approximately. Do you think Derome's assumption that this
vector can be neglected is correct?
- In section 4.2.5, it appears to me that we have reached a paradox in the
vector formalism of NMR. Remember questions 1 and 2 where we stated
that only two possible orientations are possible for spin-1/2 nuclei.
Now, it appears in Figure 4.5 that we have allowed yet a third orientation
(in the XY plane). Please explain this paradox away.
- Assuming that we now can deal with the conundrum in question 5, we should
prove to ourselves that we understand how all this precession works.
Procure a gyroscope from me and play. You need to do the following
"magnetic moment" exercises with the gyroscope (and record your
observations):
- Look at precession, prove to yourself that a higher gyromagnetic ratio
results in faster precession.
- Prove that a negative gyromagnetic ratio results in precession in the
opposite direction.
- Look at the two quantum states of nuclear magnets. Prove that
the rate of precession for both is equal.
- Align the net nuclear magnetic vector (M0) along the static
magnetic field (B0) and prove to yourself that upon
application of an X pulse, magnetization along the Y axis is
produced. Try this experiment from both X and -X as well as with
negative gyromagnetic ratio nuclei.
- Based upon your knowledge of radio-frequency pulses, explain why the
populations of the two possible nuclear magnetic quantum states are
equalized during a 90 degree pulse.
- Read carefully the material on quadrature detection and phase
cycling. Write a 4-step phase cycle which would result in half of the
desired intensity (this is a crazy example just to prove a point, one
usually wouldn't want to use such a phase cycle).