= m
= eV
= Hz


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UV Light
Beer's Law
Diode Array
Deuterium Discharge Lamp
Low Pressure Zinc Discharge Lamp
High Pressure Mercury Discharge Lamp
Low Pressure Cadmium Lamp
Tungsten Halogen Lamp
Lens and Window Material in Spectrometers
Fluorescence Reagents
Diffraction Grating
Fourier Transform IR Spectrometer
Halide Disks
Mull Samples
Film Samples for IR Spectroscopy
Light Pipes
Attenuated Total Reflectance Spectroscopy
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External Reflectance
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Photoacoustic Spectroscopy
Beam Splitter
Raman Scattering
Rayleigh Scattering
Raman Spectroscopy
Atomic Spectroscopy
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The Inductively Coupled Plasma Torch
The Helium Plasma Torch
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Atomic Absorption Spectrometry
Flame Atomic Absorption Spectrometer
Flame AA
Hollow Cathode Lamp
Electrothermal Atomization
Graphite Furnace
L’vov Platform
Electron Paramagnetic Resonance
Zeeman Effect
Continuous Wave
Electron Paramagnetic Resonance
Pulsed EPR
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Nucleus Spin Decoupling in NMR
Superconducting Magnets
NMR Microcells
Electron Impact Ionisation
Chemical Ionization
Inductively Coupled Plasma Ionization
Secondary Ion Mass Spectrometry
Fast Atom Bombardment
Plasma Desorption Mass Spectrometry
Laser Desorption Mass Spectrometry
Matrix Assisted Desorption mass Spectrometry
Field Desorption Ionization
Thermospray Ionization
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Atmospheric Pressure Ionization
Particle Beam Interface
Permeable Membrane Interface
Sector Mass Spectrometer
Quadrupole Mass Spectrometer
Ion Trap Mass Spectrometer
Time of Flight Mass Spectrometer
Optical RotationCircular Dichroism
Circularly Polarized Light
Verdet Constant
Faraday Effect

A Modern High Resolution NMR Machine Fitted with a Superconducting Magnet

Modern high-resolution NMR spectrometers must employ Superconducting Magnets to achieve and utilize homogeneous fields of 176 kGauss operating at 750 MHz for proton NMR. Superconducting Magnets are constructed with solenoids made of resistance free alloys carrying a constant and persistent current. These superconducting solenoids, however, are only superconducting at very low temperatures and to achieve these low temperatures liquid nitrogen and liquid helium baths must be employed. In addition to sample spinning, in order to obtain the necessary magnetic field homogeneity a field frequency lock is also necessary. The field is monitored by the NMR frequency of a reference substance (normally the 2H1 signal from a deuterated solvent) and any signal resulting from field drift is used in a feedback loop to correct the magnetic field back to its defined value. In addition ‘shim’ coils are employed to finally adjust the magnetic field and it is the current in these shim coils that is used to control the field homogeneity from the deuterated solvent signal. A block diagram depicting the layout of a modern NMR instrument is shown in figure 7.


Figure 7. A block Diagram Depicting the Layout of a Modern NMR Instrument

The apparatus is controlled by a computer that feeds a signal to a pulse generator, which selects pulses of high frequency radiation generated by a radio frequency (RF) generator that are then passed to a RF amplifier and thence to the coils of the sample probe. The energy absorbed provides a signal, which is amplified and passed to the detector. In the detector, the RF signal is heterodyned with the original RF source frequency and the frequency difference (now an audio frequency (AF) signal) is amplified by an AF amplifier. The output from the AF amplifier is then digitized by an analogue to digital converter (A/D converter). The digitized signal is then acquired by the computer and processed.

Superconducting Magnets require a continuous supply of current and, unfortunately, consume large quantities of cryoscopic fluids (e.g. liquid nitrogen and liquid helium ). The magnet consists of a main field superconducting coil with a number of other smaller coils that can control field gradients in different directions with respect to the main field. These smaller coils, called shim coils, are used to improve the homogeneity of the field. A modern NMR machine fitted with a superconducting magnet is depicted in figure 8.

Figure 8. TheNMR Spectrometer with a Superconducting Magnet

The superconducting coils must remain submerged in liquid helium during use, with the current in each, established during installation. Outside the liquid helium bath is a liquid nitrogen bath, which reduces the heat transfer to the helium bath, and thus conserves helium . There are liquid level sensors that actuate warning devices in both the helium and nitrogen baths to ensure they do not become exhausted. There is also a number of shim coils associated with the probe inside the magnet that operate at room temperature. These shim coils provide the final adjustments to field homogeneity, which, in modern instruments, are usually under computer control. An air supply, provided through appropriate conduits to the probe, actuates the turbine that spins the sample and also provides energy for any automatic sample handling devices.

A diagram of an NMR probe is shown in figure 9. Inside the probe is a Dewar vessel, which holds the sample tube, the various sensor coils and the conduits to the system. The Dewar is also fitted with a heater to control the probe and sample at a prescribed temperature. The Dewar contains two coils; the RF lock-coil that is usually tuned to deuterium as the reference nucleus, which, in effect, provides the calibrating scale for the Spectrum and the RF coil for the nucleus under examination. The total RF circuit is not included in the diagram to avoid confusion. There are two trimming capacitors situated in the probe, one for each of the two coils mentioned, and are adjustable from outside the probe. The probe shown is the standard type of NMR probe and cannot be used for flow through samples. In the standard instrument, the probe is not accessible from both the top and the base of the magnet but usually only from the base.

Figure 9. The Probe of a NMR spectrometer with a Super-conducting Magnet


About the Author
RAYMOND PETER WILLIAM SCOTT was born on June 20 1924 in Erith, Kent, UK. He studied at the University of London, obtaining his B.Sc. degree in 1946 and his D.Sc. degree in 1960. After spending more than a decade at Benzole Producers, Ltd. Where he became head of the Physical Chemistry Laboratory, he moved to Unilever Research Laboratories as Manager of their Physical Chemistry department. In 1969 he became Director of Physical Chemistry at Hoffmann-La Roche, Nutley, NJ, U.S.A. and subsequently accepted the position of Director of the Applied Research Department at the Perkin-Elmer Corporation, Norwalk, CT, U.S.A.
In 1986 he became an independent consultant and was appointed Visiting Professor at Georgetown
University, Washington, DC, U.S.A. and at Berkbeck College of the University of London; in 1986 he retired but continues to write technical books dealing with various aspects of physical chemistry and physical chemical techniques. Dr. Scott has authored or co-authored over 200 peer reviewed scientific papers and authored, co-authored or edited over thirty books on various aspects of physical and analytical chemistry. Dr. Scott was a founding member of the British chromatography Society and received the American Chemical society Award in chromatography (1977), the M. S. Tswett chromatography Medal (1978), the Tswett chromatography Medal U.S.S.R., (1979), the A. J. P. Martin chromatography Award (1982) and the Royal Society of Chemistry Award in Analysis and Instrumentation (1988).
Dr. Scott’s activities in gas chromatography started at the inception of the technique, inventing the Heat of Combustion Detector (the precursor of the Flame Ionization Detector), pioneered work on high sensitivity detectors, high efficiency columns and presented fundamental treatments of the relationship between the theory and practice of the technique. He established the viability of the moving bed continuous preparative gas chromatography, examined both theoretically and experimentally those factors that controlled dispersion in packed beds and helped establish the gas chromatograph as a process monitoring instrument. Dr. Scott took and active part in the renaissance of liquid chromatography, was involved in the development of high performance liquid chromatography and invented the wire transport detector. He invented the liquid chromatography mass spectrometry transport interface, introduced micro-bore liquid chromatography columns and used them to provide columns of 750,000 theoretical plates and liquid chromatography separations in less than a second. Dr. Scott has always been a “hands-on” scientist with a remarkable record of accomplishments in chromatography ranging from hardware design to the development of fundamental theory. He has never shied away from questioning “conventional wisdom” and his original approach to problems has often produced significant breakthroughs.

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