1 / 35

Design, Care and Feeding of NMR Probes: A Tutorial

Design, Care and Feeding of NMR Probes: A Tutorial. 2011 Experimental NMR Conference, Asilomar CA. sources of inspiration. Don Alderman Mark Conradi David Hoult Bob McKay Eichii Fukuskima David Doty Toby Zens Frank Engelke Allen Palmer John Stringer . . . .

guang
Download Presentation

Design, Care and Feeding of NMR Probes: A Tutorial

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Design, Care and Feeding of NMR Probes: A Tutorial 2011 Experimental NMR Conference, Asilomar CA

  2. sources of inspiration.... Don Alderman Mark Conradi David Hoult Bob McKay Eichii Fukuskima David Doty Toby Zens Frank Engelke Allen Palmer John Stringer . . . . and many, many, many others too numerous to mention .... David Hoult Mark Conradi Don Alderman David Doty Eichii Fukushima Bob McKay Toby Zens

  3. Design, Care and Feeding of NMR Probes: A Tutorial Part I What is a tank circuit? Impedance matching transmission lines the Smith chart experimental techniques Circuit resonance Q and voltage rise arcing and avoiding arcing Part II Signal to noise Rf efficiency comparing specifications Circuit balancing and multiple resonance circuits Finite element field simulations Tuning tube and transmission line probes

  4. Disclaimer: semi-professional driver on a closed track. Do not attempt at home. The "management" of ENC is not responsible for damages as a result. Opinions of the speaker do not reflect those of the ENC unless you happen to like them, and in that instance ENC takes full credit.. "it is easier to repent than it is to get permission" - D. M. Grant

  5. signal emf = - NMR probe basics resonator An NMR probe is a tank circuit used to excite NMR signals and detect them by Faraday induction RF input impedance matching network

  6. Bo N S B1(t) Resonators...type usually dictated by sample geometry and frequency Solenoidal coil Saddle coil all resonators are inductive elements slotted tube scroll coil Zens resonator bird cage

  7. primitive probe transmission line RF input resonator very inefficient because of impedance mismatch RF signals have wave character and require phase matching

  8. n1 n2 Impedance matching of light waves index of refraction n1 for p-polarized light the transmission coefficient depends on n1, n2 and the incident angle θ. index of refraction n2 R = 0 and T = 1 when

  9. DC electronics basics – Ohm's Law V R V C V L V = IR RF electronics – Ohm's law works using Impedance V(t) = Vocos(ωt + φ) or V(t) = Re(ej(ωt +φ))

  10. RF electronics basics – Impedance and Reactance V R V C V L V = IZR V = IZC V = IZL from V(t) = ej(ωt +φ) ZR = R Define a complex impedance Z ZC = 1/jωC ZL = jωL Z = R + jX X = Reactance

  11. Transmission lines and characteristic impedance Can't just connect a load to a source with a wire – it will radiate the power ρ = | Γ | • The voltage standing wave ratio is then equal to: Dipole antenna radiates power from transmitter into space To transmit RF to a load need a structure to contain the EM waves

  12. for dielectric Transmission lines and characteristic impedance twin-line d b coaxial line length l characteristic impedance Zo is the equivalent of a refractive index Minimum attenuation cable: if εR = 1.0, Zo = 75Ω; εR = 2.0, Zo = 51Ω

  13. VSWR = Vmax/Vmin = (1 + |ΓL|)/(1 − |ΓL|) reflection coefficient if ZS = Zo = 50 Ω ZL = 50 Ω ZL = 25 Ω Vinc Vinc Vref Vref VSWR = 1 VSWR = 2 Vinc Vinc Vrefout of phase 180o for short Vrefin phase for open VSWR = ∞ VSWR = ∞

  14. Impedance matching the coil R set X = 0 to find allowed ω there will be 2 ! Then choose CT/CM to render R' = Zo resonant frequency ω ~

  15. easier to use a Smith chart 50Ω Example: match a 200Ω load L 200Ω C load 200Ω VSWR = 0

  16. Measuring 1 Spectrum analyzer + tracking generator DUT 0 frequency matched RF receiver RF output Forward wave directional coupler reflected wave 50Ω

  17. Resonator inductance for solenoid length , diameter d, n turns dimensions in inches usually more practical to measure L

  18. Resonant RLC circuits when ω2 = 1/LC the circuit is "resonant" RF energy at ω is stored alternately in C and L Circuit can be excited by an antenna or other source

  19. Zo Zo Zo Using resonance to span a break in a transmission line circuit

  20. Zo Zo Zo Using resonance to span a break in a circuit L C

  21. Impedance matching the coil R set X = 0 to find allowed ω there will be 2 ! Then choose CT/CM to render R' = Zo resonant frequency ω ~

  22. Measuring Spectrum analyzer + tracking generator DUT frequency RF receiver RF output Forward wave directional coupler reflected wave 50Ω

  23. Voltage at circuit resonance when ω2 = 1/LC Zin = R and |XC| = |XL|I = Vin/Zin = Vin/R What is the voltage VH – Vin across C?

  24. Coil quality factor Q =ωL/R = E stored/E dissipated per cycle = ω/3dB bandwidth typical Q ~ 100 or more Input pulse power Peak V across C ~ 10,000 V !!! Vptp

  25. Conditions for arcing through air

  26. Non-magnetic fixed and variable capacitors 500V Vacuum variable 2.5 kV 20 kV Sapphire trimmer 10 kV RF transmitting ceramic chips 2.5 kV Teflon variable

  27. Probe testing under power Directional coupler output forward reflected Power amplifier

  28. Probe testing under power arcing Directional coupler output reflected forward Power amplifier

  29. Arc testing • tune and match at low power • increase drive 1 dB at a time while watching reflected power • operate 2 dB lower than initial arc • avoid hard sustained arcing – carbonized capacitors do not heal • don't try and rematch to compensate for arcing

  30. Always make sure you have air flow into the probe

  31. Dewar's frequently provide sources of arcing If the probe only arcs in the magnet suspect the dewar

  32. signal emf = - = B1 from unit current Part II.......maybe for next year Optimizing RF efficiency and S/N "principle of reciprocity" Excitation and detection are equally efficient

  33. Acknowledgements • For inspiration and graphics • Abragam • D. VanderHart • M. Conradi • T. and H. Barbara • T. Zens • D. Alderman • B. Mckay • Palmer • J. Stringer • F. Engelke • G. Facey • J. Daniels • E. Fukushima • D. Doty L. Page S. Brin S. Wolfram J. Wales J. Hornak R. Schurko For support NSF ExxonMobil Agilent Yale University all of my present and former students

  34. Disclaimer: semi-professional driver on a closed track. Do not attempt at home. The "management" of ENC is not responsible for damages as a result. Opinions of the speaker do not reflect those of the ENC unless you happen to like them, and in that instance ENC takes full credit.. "your students only learn your worst habits" - C. P. Slichter

More Related