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Pulsed/CW NMR
Pulsed CW NMR

TeachSpin's Pulsed/CW NMR Spectrometer, PS2-A, is a versatile, sensitive, rugged and reliable nuclear magnetic resonance spectrometer designed specifically for instruction. Any exploration of the capabilities of this apparatus easily explains the title of our introductory newsletter "Pulsed NMR on STEROIDS."

Overview of the PS2-A System
Hands-On Advantages
Analog Outputs Will Never Be Obsolete
Single Coil Sample Probe
NMR Signals of both Hydrogen and Fluorine Nuclei
Gradient Field Coils Optimize Homogeneity
Proprietary Temperature Controller
Investigations Using Fast Fourier Transforms (FFT)
Pulse Programmer/Spin-Echoes
NMR of "Soft" Solids
Using the Apparatus for Continuous Wave (CW) NMR


Overview of the PS2-A System
  • High-Field, High Homogeneity Permanent Magnet
    • 0.49 Tesla, 21 MHz proton resonance
    • field stabilized to 1 part in 106 over a 20 minute interval.
  • RF sample probe with
    • single coil and a 50 ohm input impedance; a matched unit.
    • four independently adjustable gradient coils (x, y, z, z2) available to:
      • enhance homogeneity
      • provide known gradients for diffusion measurements and one dimensional imaging
  • PS2 Controller containing
    • dedicated current regulated supply for each of the four gradient coils
    • magnet temperature controller
  • Mainframe with Four Electronic Modules
    • pulse programmer
    • synthesizer including both oscillator and pulse amplifier
    • receiver with both envelope detector and quadrature phase sensitive detector
    • lock-in/field sweep with detector

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Hands-On Advantages

The specifications of this unit rival any research grade unit in this frequency range in terms of sensitivity, stability, capabilities and state- of-the-art electronics. PS2-A was, however, designed from the outset for student instruction. Students, and not a computer, adjust the shim coils and set all of the experimental parameters. They can make many informative mistakes including miswiring the spectrometer and incorrectly setting any and all of the parameters without damaging the unit. For the one case where incorrect wiring might do some damage, the unit has special connectors which make those connections impossible.

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Analog Outputs Will Never Be Obsolete

All of the data is presented in analog form for examination on a digital storage oscilloscope or a computer. Students (and faculty) can then choose how they wish to perform data reduction or analysis. No proprietary software programs are needed to operate the unit, so no software updates are needed.

TeachSpin is convinced that the "volt" will never go out of style, and that the mode of data storage and analysis is a choice best left to the individual user. Although data storage and analysis hardware and software is changing so rapidly that what is "hot" today may be obsolete tomorrow, your TeachSpin spectrometer, with its analog output signals, will be capable of taking research grade data long into the future.

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Single Coil Sample Probe

Unlike our original PNMR spectrometer, PS2-A is a single coil, matched sample probe instrument. There are many advantages to a single coil unit; including lower power required for RF pulses, smaller size, smaller magnet gap, and an impedance matched sample probe.

For a student, however, operation of the single coil system may appear to be pure "magic". There are many ways to accomplish this "magic", but we have chosen a system that can be readily understood by a beginner. The block diagram is shown below

The instruction manual devotes several pages, with several diagrams, to explain carefully and clearly how this single coil system works for both pulsed and CW resonance. The "magic" turns out to be clever electronics.

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Using the Apparatus for Pulsed NMR

NMR Signals of both Hydrogen and Fluorine Nuclei

Using PS2-A, students can observe NMR signals from two types of nuclei, hydrogen (proton) and fluorine. This opens up the possibility of studying an entirely new collection of molecules in liquids and some solids. Fluorine nuclei are particularly interesting because they typically exhibit large chemical shifts in various compounds. In our original spectrometer, PS1-A, where only proton NMR could be studied, the small chemical shifts were not observable. This was a deficiency, especially for the chemistry faculty. One might even say that chemical shifts are the bread and butter of organic chemistry's NMR analysis. Now, with this unit, chemical shifts in fluorine compounds are easily observable and some can even be seen in proton compounds.

The reason these "splittings" are observable in PS2-A is not just the fact that it can detect fluorine NMR, but also that the new unit has a larger and more homogeneous magnetic field. The proton resonant frequency is 21 MHz and we have observed T2* as long as 25 milliseconds in some magnet using the electric gradient field coils.

Gradient Field Coils Optimize Homogeneity
Four sets of gradient field coils are built into the RF sample head, each of which is controlled by its own current regulated power supply. Because they offer control of the x, y, z, and z2 gradients, students can adjust these coils to increase, significantly, the homogeneity of the magnetic field over the sample.

The screen capture on the right shows two free induction decays for the same distilled water sample. The upper trace was taken with the gradient coils off while the lower trace was taken with the gradient coils adjusted for optimum homogeneity.

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Two FID for Distilled Water showing the effect of increased homogeneity created by gradient coils

Proprietary Temperature Controller

Not only has the magnetic field been increased in magnitude and homogeneity, it has also been greatly enhanced in stability. Magnetic field stability has been a problem with permanent magnets because the magnetization of the NdFeB alloys is extremely temperature dependent. Our original spectrometer needed to be retuned every five to ten minutes and thus RF phase sensitive detection was impractical. After its forty-five minute warm-up period, PS2-A has a field stability of one part in 106 over fifteen minutes. This is accomplished with a proprietary magnet design and PID temperature controller. Both the temperature controller and the current regulated supplies for the gradient coils are housed in the hardwood case that is shown on top of the Mainframe of the instrument.

With such outstanding field stability, students can take advantage of data from the two channel quadrature RF phase sensitive detection. The reference RF has a full 360° phase shift with one degree resolution. There is also an envelope detector as well as a buffered output of the direct RF magnetic resonance signal. Again, because of the field stability, students can perform long term signal averaging with the phase sensitive detector signals, to extract weak signals from noise. Such signal averaging is now a standard feature on almost all digital oscilloscopes.

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Investigations Using Fast Fourier Transforms (FFT)
This new high-homogeneity, high-field magnet allows students to use the modern form of spectroscopy Fast Fourier Transforms (FFT) for both fluorine and proton samples. The oscilloscope screen shows the FID signals of a liquid called Fluorinert, FC-70, with the envelope detector (on resonance) and a RF phase sensitive detector slightly off resonance.

This sample shows a dramatic beat structure, indicating the presence of at least two inequivalent fluorine sites in the sample.
FID for Fluorinert FC-70


This screen capture shows the FFT of the phase detector signal, which has been signal averaged over 16 pulses. The FFT spectrum indicates the presence of three inequivalent fluorine sites and gives their relative splittings.

The spectrometer is shipped with a set of four different fluorine liquids, all of which are safe for student use.

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FFT for Fluorinert FC-70 showing three inequivalent fluorine sites.

Pulse Programmer/Spin-Echoes
The Pulse Programmer Module of the Mainframe provides a wide variety of pulse sequences. All pulse widths and time delays are digitally generated for stability and accuracy. A simple two pulse π/2 - π spin-echo combination for light mineral oil is shown. The narrow spike is the π pulse which then leads to the single spin echo. Students can vary not only the pulse width but also the delay time between pulses and the repetition time for the sequence.

Students can determine spin-lattice relaxation time (T1) in any sample by systematically varying the delay time between the two pulses of a π - π/2 sequence.
Initial FID and spin-echo of Light Mineral Oil for a π/2 - π pulse sequence.

Multi-pulse combinations are available in both Carr-Purcell and Meiboom-Gill (MG) sequences. A toggle on the Pulse Programmer module allows students to switch the MG on and off so that they can see how using this sequence enhances their data. The figure at the right shows a thirty p-pulse MG sequence used to measure spin-spin relaxation time (T2) in light mineral oil.

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Thirty p-pulse MG spin echo signal

NMR of "Soft" Solids
Our new unit has a significantly reduced recovery time after the pulse. This allows the spectrometer to measure signals from many "soft" solids which have T2 longer than ten microseconds. Here we see the FID signal for fluorine nuclei in Teflon. Rubber, greases, plastics and other solid materials with either hydrogen or fluorine nuclei can be studied. With a recovery time of the order of 15 µs, an entire class of solids can now be added to the long list of candidates for exploration.

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FID for Fluorine Nuclei in Teflon


Using the Apparatus for Continuous Wave (CW) NMR

Over the years, we have consistently had requests for an instrument that could detect magnetic resonance signals not only using pulsed NMR but also using the original continuous wave (CW) spectroscopy, so that students could study the relationship between them. That is exactly what we have accomplished. This unit is capable of observing NMR signals for either hydrogen or fluorine nuclei using a continuous RF field and sweeping the magnetic field through resonance.

A built-in two channel fixed modulation frequency lock-in amplifier is used for enhancing the CW signals for broad linewidth signals. It allows students to gain first hand experience with lock-in detection in NMR. The lock-in module also provides the current for the magnetic field sweep coils as well as an output analog voltage proportional to the field sweep. Various sweep times, sweep ranges, field offsets, voltage amplification, and low-pass time constants are available in the unit.

This oscilloscope screen capture shows the CW resonance signals for the fluorine FC-70 Fluorinert liquid. This signal came from the RF phase sensitive detector with no attempt to separate the real and imaginary part of the nuclear susceptibility using the phase shifter. However, the magnetic field splittings observed in the CW spectrum can now be compared to the frequency splittings detected in the FFT spectrum of the free induction decay. After performing both experiments, it should become clear to the students why the modern spectrometers all use the FFT analysis of the FID.

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