When comparing two NMR spectra, always keep in mind the subtle differences in the way the spectra were recorded. One obvious example is the effect of field strength. As the Bo field increases in magnitude (i.e. 1.5T, 4.7T, 7T) the signal-to-noise ratio generally increases. The shape of the spectrum may also change. For example, consider the hydrogen NMR spectrum from three coupled nuclei A, B, and C with the following chemical shifts and J coupling constants.
Compare the 100 MHz and 400 MHz NMR spectra. The spectral lines from the B type spins are colored red. You can see how easy it would be to make the wrong choice as to the structure of the molecule based on the 100 MHz spectrum, although the chance of error might be reduced if you had further information, eg. the relative areas under the peaks. This topic is described in a later section of this chapter.
Most routine high resolution NMR samples are prepared and run in 5 mm glass NMR tubes. Always fill your NMR tubes to the same height with lock solvent. This will minimize the amount of magnetic field shimming required. The animation window depicts a sample tube filled with solvent such that it fills the RF coil.
The concentration of your sample should be great enough to give a good signal-to-noise ratio in your spectrum, yet minimize exchange effects found at high concentrations. The exact concentration of your sample in the lock solvent will depend on the sensitivity of the spectrometer. If you have no guidelines for a specific spectrometer, use one drop of analyte for liquids and one or two crystals for solid samples.
The position of spectral absorption lines can be solvent dependent. Therefore, if you are comparing spectra or trying to identify an unknown sample by comparison to reference spectra, use the same solvent. The hydrogen NMR spectrum of ethanol is a good example of this solvent dependence. Compare the positions of the CH3, CH2, and OH absorption lines in a hydrogen NMR spectrum of ethanol in the lock solvents CDCl3 and D2O . Notice also that the relative peak heights are not the same in the two spectra. This is because the linewidths are not equal. The area under a peak, not the height of a peak, is proportional to the number of hydrogens in a sample. This point will be emphasized later in this chapter.
Variations in the polarity and dielectric constant of the lock solvent will also effect the tuning of the probe. The correction of these effects are covered in the next section of this chapter on sample probe tuning.
Most spectrometers have a probe tuning mode of operation. This mode of operation presents a display of reflected power vs. frequency on the screen. The goal is to adjust the display so that the reflected power from the probe is zero at the resonance frequency of the nucleus you are examining.
As the polarity and dielectric constant of the lock solvent changes, so does the bandwidth of the RF probe. This is significant because it affects the amount of RF power needed to produce a 90 degree pulse. The larger the bandwidth, the more power is needed to produce the 90 degree rotation.
To determine the pulse width needed to produce a 90 degree pulse, you should perform the following experiment using a sample which has a single absorption line and a relatively short T1. Record a series of spectra with incrementally longer RF pulse widths. Fourier transform the time domain signals and plot these lines as a function of pulse width. The peak height should vary sinusoidally with increasing pulse width. The 90 degree pulse width will be the first maximum. The 180 degree pulse width will be the first zero crossing. Many spectrometers have routines which will automatically record the data necessary to produce these plots.
You should also be aware of the effect of varying the width of the RF pulse on the distribution of frequencies being delivered to your sample. Recall from the discussion of the convolution theorem in Chapter 5 that the Fourier pair of a sine wave which is turned on and off is a sinc function centered at the frequency of the sine wave. When you apply an RF pulse of width t in the time domain, you apply a distribution of frequencies to your sample. Not all of these frequencies will have sufficient B1 magnitude to produce a 90 degree rotation. The range of frequencies from the center of the distribution to the first zeros in the distribution is +/- 1/t. As your pulse width increases, the width of the distribution of frequencies in your pulse decreases. If the distribution is too narrow, you may not be applying the desired rotation to the entire sample.
Broad lines, asymmetric lines, and a loss of resolution are indications that a magnet needs to be shimmed. The shape of an NMR line is a good indication of which shim is misadjusted. Consider a single narrow NMR line. If we zoom in on this line we might see the following shape. . The following series of spectra depict the appearance of this spectral line in the presence of various inhomogeneities.
In general, asymmetric lineshapes result from mis-adjusted even-powered Z shims. This can be seen by looking at the shape of a Z2 shim field. As you go further away from the center of the sample in the +Z or -Z direction, the field increases, giving more components of the spectral line at higher fields. The higher the power of the Z inhomogeneity, the further away the asymmetry is from the center of the line.
Symmetrically broadened lines are from mis-adjusted odd-powered Z shims. Consider the shape of the Z3 shim field. The top of the sample (+Z) is at a higher field, resulting in higher field spectral components, while the bottom (-Z) is at a lower field, giving more lower field spectral components. Transverse shims (X,Y) will cause large first order or second order spinning sidebands when the sample is spun. The shape of these inhomogeneities cause the sample, when it is spun, to experience a periodic variation in the magnetic field. Those shims (XY or X2-Y2) causing a spinning sample to experience two variations per cycle will create second order spinning sidebands.
Electronic amplifiers often have small offsets in their output when no signal is being put in. This is referred to as the DC offset of the amplifier. A DC offset in the time domain is equivalent to a peak at zero frequency in the frequency domain. If there is an FID on top of a DC offset, its Fourier transform will have an additional peak at zero frequency in the spectrum. This picture has been simplified by presenting only the real part of the signal.
The DC offset could be eliminated by spending thousands of dollars on better quality amplifiers. Alternatively, the artifact can be removed by taking an FID recorded with a 90 degree pulse applied along +X' , an FID recorded with a 90 degree pulse applied along -X' (note the phase change in the FID) , multiplying the FID recorded with a 90 degree pulse along -X' by -1 , adding the two FIDs, and Fourier transforming. This process only costs a little extra time and a few extra lines of computer code.
Another type of artifact is caused by having unequal gains on the real and imaginary outputs of the quadrature detector. For a Fourier transform to produce a proper spectrum, it requires true real and imaginary inputs. When the inputs are equal in amplitude, there are no negative frequency artifacts in the spectrum. If the two inputs are different, the negative frequency components of a signal do not cancel. You can tell a negative frequency artifact because it appears to be the mirror image (but smaller) of a peak from the opposite sign end of the spectrum.
Negative frequency artifacts can be removed by recording an FID with Mx or the real signal (My or the imaginary signal) from channel 1 (2) of the quadrature detector. Another FID is recorded with Mx or the real signal (My or the imaginary signal) from channel 2 (1) of the quadrature detector. The two FIDs are then averaged. As a result, the amplitude of the real and imaginary inputs to the FT are equal, so when the FIDs are Fourier transformed, there are no negative frequency artifacts.
The averaging described above can be achieved by applying a 90 degree pulse about +X and a 90 degree pulse about +Y, and adding the two resulting FIDs together. To eliminate all possible errors from different combinations of these types of pulses, phase cycling is applied. Phase cycling adds together eight FIDs recorded with the following phases to eliminate all the possible quadrature artifacts.
Once an FID is recorded and Fourier transformed, the resultant spectrum must be phased so that all the absorption lines are positive. You are encouraged to review Chapter 5 for an explanation of the need to phase correcting a spectrum. There are various automatic and manual phase correction algorithms on most NMR spectrometers.
Here are a few examples of simple hydrogen NMR spectra to demonstrate the capabilities of NMR spectroscopy. As you become more knowledgeable about NMR, you will learn the relationship between peak locations, peak splitting, and molecular structure in NMR spectra.
||methyl ethyl ketone||CH3(C=O)CH2CH3||CDCl3 ||water||H2O ||D2O
||1-propanol||CH3CH2CH2OH || CDCl3
||2-propanol||(CH3)2CHOH || CDCl3
||t-butanol||(CH3)3COH || CDCl3
||2-butanol||CH3CH2CH(OH)CH3|| CDCl3 ||pyridine||C5H5N|| CDCl3
Consider the methyl ethyl ketone (CH3CH2(C=O)CH3) molecule and its hydrogen NMR spectrum. When the -CH2- ( = 2.25 ppm), -CH3 ( = 2.0 ppm), and CH3- ( = 0.9 ppm) peaks are integrated we get the following spectrum. The areas under the three types of peaks on this spectrometer are 26:39:39. Dividing each number by 13, we obtain a 2:3:3 ratio which is proportional to the number of -CH2- to -CH3 to CH3- hydrogens.
There are a few assumptions which were made in presenting this rule.
You may correct for a sloping baseline by performing a baseline correction to the spectrum. A poor signal-to-noise ratio may be improved by performing signal averaging, discussed next.
Because of the need to perform phase cycling, you will need to have the number of averages equal to a multiple of the minimum number of phase cycling steps. Compare the results of averaging together the following number of spectra of a very dilute solution of methyl ethyl ketone.
When filling the magnet with liquid nitrogen, you must be sure not to exceed the recommended fill pressure and rate for your magnet. If your magnet has two liquid nitrogen ports, one should be used for filling and the other for venting the boil-off gaseous nitrogen and overfill liquid nitrogen. A piece of tubing is typically placed on the vent port to direct the overfill liquid nitrogen away from the magnet seals, probe, and electronics. It is highly recommended that your liquid nitrogen tanks be made of non-magnetic stainless steel.
Liquid helium fills are typically a two-person operation. Because they are done so infrequently, it is good to review the process before each fill. The fill requires a supply dewar of liquid helium, a special liquid helium transfer line, and a tank of pure compressed helium gas. Liquid helium is transferred from the liquid helium supply dewar up through the transfer line, into the helium dewar of the magnet.
The transfer line goes into the top of the liquid helium supply dewar, but should never rest on the bottom of the dewar. The bottom of the dewar may contain frozen water, oxygen, and nitrogen which will be forced into your magnet if the transfer line touches the bottom during the transfer process. The compressed helium gas, mentioned earlier, is for pressurizing the liquid helium supply dewar with about 2 to 4 psi of pressure. Gauges on helium supply dewars can be very inaccurate, so do not count on them to give you an accurate reading. A helium pressure above the liquid forces the Helium into the magnet dewar.
The transfer line is usually inserted into the magnet until it contacts a transfer flange in the bottom of the magnet. The nitrogen ports on the magnet should be plugged with a check valve during filling of the helium dewar of the magnet. This step prevents cryopumping, a process whereby nitrogen, water, and oxygen are condensed out of the atmosphere into the nitrogen dewar due to the magnet stacks being cooled by the helium. Many labs loosely plug the helium vents with tissue during the fill. This cuts down on cryopumping should the flow of the venting He drop.
The best way to determine if the magnet is full is to look for a change in the gas cloud coming out of the magnet vents. When the magnet is full the cloud becomes very thick with a deep white center plume with a slight blue tint. The helium vents on the magnet should be closed promptly after the magnet is full.
The UNIX file system is divided into directories, which are equivalent to folders in some operating systems. Because UNIX is a multi-user system, there must be a way to keep your directories separate (and safe) from someone else's. To achieve this, there are accounts with passwords and ownership of directories. For example, you have an account which has a password. Logging on under your account gives you access to your directories and to other directories for which you have access (permission).
The most useful, but least used command in UNIX is man. This is short for manual and gives you on-line help on every UNIX command. The more you use it, the easier it is to use. The animation window contains a table of a few simple UNIX commands. Entries in italics are examples and can be any string of characters or numbers.
Copyright © 1997-2017 J.P. Hornak.
All Rights Reserved.