design, care and feeding of nmr probes: a tutorial 2011 experimental nmr conference, asilomar ca
TRANSCRIPT
Design, Care and Feeding of NMR Probes: A Tutorial
2011 Experimental NMR Conference, Asilomar CA
sources of inspiration....
Don AldermanMark ConradiDavid HoultBob McKayEichii FukuskimaDavid DotyToby ZensFrank EngelkeAllen PalmerJohn Stringer....
and many, many, many others too numerous to mention ....
Don Alderman
Mark ConradiDavid Hoult
Bob McKayEichii Fukushima
David Doty
Toby Zens
Design, Care and Feeding of NMR Probes: A Tutorial
Part I
What is a tank circuit?
Impedance matchingtransmission linesthe Smith chartexperimental techniques
Circuit resonanceQ and voltage risearcing and avoiding arcing
Part II
Signal to noiseRf efficiencycomparing specifications
Circuit balancing and multiple resonance circuits
Finite element field simulations
Tuning tube and transmission line probes
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
NMR probe basics
An NMR probe is a tank circuit used to excite NMR signals and detect them by Faraday induction
CT L
CM
Z O
resonator
RF input
impedance matching network
+-
v ( t )
L
signal emf = -
s
1V
d(B M(t))dV
dt
Solenoidal coil
B1(t)
Bo
Saddle coil
slotted tube
scrollcoil
Zensresonator
birdcage
all resonators are inductive
elements
Resonators...type usually dictated by sample geometry and frequency
N
S
transmission lineRF
inputresonator
primitive probe
very inefficient because of impedance mismatch
RF signals have wave character and require phase matching
index of refraction n1
index of refraction n2
for p-polarized light the transmission coefficient depends on n1, n2 and the incident angle θ.
Impedance matching of light waves
R = 0 and T = 1 when
1 1
B2
nn
-θ tan
n1 n2
DC electronics basics – Ohm's Law
V
V = IR
V
dVI =C
dt dIV =L
dt
RF electronics – Ohm's law works using Impedance
V(t) = Vocos(ωt + φ) or V(t) = Re(ej(ωt +φ))
VR C L
RF electronics basics – Impedance and Reactance
V
V = IZR
V
from V(t) = ej(ωt +φ)
V = IZC
V = IZL
ZR = R
Z = R + jX
Define a complex
impedance Z
ZC = 1/jωC
ZL = jωL
X = Reactance
VR C L
j = 1
Transmission lines and characteristic impedance
Can't just connect a load to a source with a wire – it will radiate the power
Dipole antenna radiates power from transmitter into space
To transmit RF to a load need a structure to contain the EM waves
Transmission lines and characteristic impedance
twin-line
coaxial line
characteristic impedance Zo is the equivalent of a refractive index
L o
in oo L
Z jZ tan(βl)Z (l) Z
Z jZ tan(βl)
length l
2πβ
λ
μη
ε for dielectric
o
ηZ ln(b/ a)
2π
b
do
ηZ ln(d/ a)
2π
Minimum attenuation cable: if εR = 1.0, Zo = 75Ω; εR = 2.0, Zo = 51Ω
ZL = 50 Ω
refl ected L s
L sincident
V Z ZΓ
V Z Zreflection coefficient
VincVinc
Vinc Vinc
VrefVref
Vref out of phase
180o for short
Vref in phase
for open
ZL = 25 Ω
if ZS = Zo = 50 Ω
VSWR = Vmax/Vmin
= (1 + |ΓL|)/(1 − |ΓL|)
VSWR = 1
VSWR = ∞ VSWR = ∞
VSWR = 2
Impedance matching the coil
in o m
T
1Z Z jωC R' jX
1jωL R
jωC
CT L
CM
Z O
R
set X = 0 to findallowed ω
there will be 2 !
Then choose CT/CM
to render R' = Zo
resonant frequency ω ~ T1/ LC
easier to use a Smith chart
VSWR = 0
50Ω
200Ω
L
C
load 200Ω
Example: match a 200Ω load
Measuring
Spectrum analyzer + tracking generator
RF outputRF receiver
directional coupler
Forward wave
DUT
reflected wave
50Ω
frequency
matched
Γ
Γ
0
1
Resonator inductance
for solenoid length , diameter d, n turns
22 d
L 250n (nH)4.5d 10
usually more practical to measure L
dimensions in inches
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
C
L
R
Zo
Zo
Zo
Using resonance to span a break in a transmission line circuit
Zo
Zo
Zo
Using resonance to span a break in a circuit
C
L
2
1plot vs. C
ω
Impedance matching the coil
in o m
T
1Z Z jωC R' jX
1iωL R
jωC
CT L
CM
Z O
R
set X = 0 to findallowed ω
there will be 2 !
Then choose CT/CM
to render R' = Zo
resonant frequency ω ~ 1/ LC
Measuring
Spectrum analyzer + tracking generator
RF outputRF receiver
directional coupler
Forward wave
DUT
reflected wave
50Ω
frequency
Γ
Voltage at circuit resonance
C LV in
V H R
in
1Z = +jωL+R
jωC
j = - +jωL+R
ωC
when ω2 = 1/LC Zin = R and |XC| = |XL| I = Vin/Zin = Vin/R
What is the voltage VH – Vin across C?
L inc in inH in c in
| Z | V| Z | V ωLVV V | Z | I QV
R R R
Coil quality factor Q =ωL/R = E stored/E dissipated per cycle = ω/3dB bandwidth
typical Q ~ 100 or more
Input pulse power
2 2 22
ptp ptpRMSptp
o o
(V / 2 2) VV100 Watts V 200V
Z Z 400
Vptp
Peak V across C ~ 10,000 V !!!
Conditions for arcing through air
Non-magnetic fixed and variable capacitors
20 kV
10 kV
500V
2.5 kV
2.5 kV
Vacuum variable
Teflon variable
Sapphire trimmer
RF transmittingceramic chips
Probe testing under power
Power amplifier
Directional coupler output
forward reflected
Probe testing under power
Power amplifier
Directional coupler output
forward
arcing
reflected
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
Always make sure you have air flow into the probe
Dewar's frequently provide sources of arcing
If the probe only arcs in the magnet suspect the dewar
Optimizing RF efficiency and S/N
signal emf = -
s
1V
d(B M(t))dV
dt
1B= B1 from unit current
"principle of reciprocity"
Excitation and detection are equally efficient
o 1xy o s oemf ωB M V (cosω t)
2 2o o sM Nγ I (I 1)B / 3kT
2o
1
1
emf B
emf B / unit current
B / power
Part II.......maybe for next year
Acknowledgements
For inspiration and graphics
A. AbragamD. VanderHartM. ConradiT. and H. BarbaraT. ZensD. AldermanB. MckayA. PalmerJ. StringerF. EngelkeG. FaceyJ. DanielsE. FukushimaD. Doty
L. PageS. BrinS. WolframJ. WalesJ. HornakR. Schurko
For support
NSFExxonMobilAgilentYale University
all of my present and former students
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