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# T. a) B( }' a/ I! ACross-talk between FM Broadcast Radio Transmitters (88-108 MHz)' I: G8 i+ j) l$ Q, f# S( j( P
and NMR Spectroscopy: A recent experience
4 \+ B4 T1 x7 X# W/ S! a2 ^( c# S* r
& \( m# G, O+ xRecently I had to install a 400 MHz (9.4 T) NMR Spectrometer. The
) W i$ L# p. Dsystem worked fine and, using an Indirect Detection Probe , met quickly4 R2 n& S- l* j8 [
and effortlessly the specifications. But later on, when the customer/ @5 v# H- v/ s3 V
installed a 13C direct detection Probe, the S/N ratio turned out to be
! J% j1 s3 c$ tquite low and, on top of it, the sensitivity was subject to erratic and
& D1 G9 m2 F( l4 Rvery large variations from 50:1 to 130:1 (manufacturer's specs give
' U. h' D+ \5 n4 g155:1), without any apparent reason.$ |/ [$ }" \8 @+ g" V
Since the nominal 13C observe frequency at 9.4 T is 100,568
Y& r4 i6 C+ H" dMHz, right in the middle of the range of commercial FM broadcasts, I" V3 L* D t. h0 E9 t6 `! j) q
have immediately suspected that the spectrometer was picking up one of8 r+ p5 A- x# F% } [+ q
those radio stations. In fact, using a cheap FM radio receiver, a
* r8 v. H8 P. y' B# d9 istrong station was quickly found at 100,60 MHz. At this point, I have |) G0 E$ b/ V# D6 L
connected a simple audio amplifier ending with a loudspeaker to the
7 O" g/ e4 S- z5 l' v$ Routput BNC of the observe receiver which was there apparently just for; S( [5 @2 [/ N, {$ W2 Q4 W9 t
this purpose, and all of us were listening to the radio using a 200.000
3 [/ ?6 G: o8 D% HEuro NMR spectrometer, except that the audio quality was really poor,) K/ O# N8 D. a+ H# v' d! `8 K
much worse than from the above-mentioned gadget radio (a shopping mall0 \* l8 P6 u. x# Z4 A# k8 A2 l7 r
gift).
% V* Q. ]- p; X1 l: ]3 c The problem is well known from the old times, when the highest* a8 S! A: ^1 V+ u E6 z' T
field was 2.45 T and the nominal H1 frequency was close to 100 MHz. One9 ~# W6 \ @2 i; d
of the first Italian NMR spectroscopists to experience it, back in
5 e4 z# i9 g; F9 `! [' J4 }4 a+ c2 ?1974, was Prof. L.Lunazzi at University of Bologna, on his brand new# L* F1 e% r) M3 D9 p$ A
Varian XL100 spectrometer, and the radio station was Radio San Luchino,
& |3 o' O6 a* fwell known to anybody living in Bologna, which broadcasts from the top: S2 U" N# N% v" C7 E3 y
of the nearby Saint Luca hill.$ A; h$ }) B( d8 Z
The obvious solution is to change the magnetic field, and thus0 m4 D8 b4 ? {; y
all resonance frequencies, in order to get out of the modulation1 c. C( `+ o; |$ q1 T
envelope of the interfering transmitter. But this is not always easy,9 Y! {& l8 |) y( E
since the range by which one can move the magnetic field changing just
, ~) x2 P9 ~: g/ U5 S$ k; n8 w2 }2 [some software parameters is usually limited to a few tens of kHz in the
6 H' a: k4 Q/ }% X" d7 Pfrequency domain. If larger variations are required the poor engineer
* S! \8 Q) w1 `* _' {has to work on the superconducting coils of the magnet, which is a
! e# O' Z E7 E) p8 Qno-trivial job entailing the risk of a total or partial quench. ^$ h7 f# I. p5 ? k8 C5 e
Bitter experience shows that persuading the involved radio
5 e& `$ O3 p& Z. Q7 Astation to change its operating frequency is a time consuming,
6 e* M/ n' H- U' j" ?1 pfrustrating, and apparently quite impossible task.
1 `, ?- j5 i9 M Being well aware of the problem, my preliminary spectrometer
- H3 O, Y3 P, P7 |; S Pchecks always include some blank acquisitions taken before running up) f1 o; C" l i8 A& Z2 N& M% T
the magnet so that there is no chance to observe an NMR signal. The
& J+ z/ y2 J( l S6 |1 Vresulting dataset should be pure white noise, without significant4 W1 Y0 _) K l3 R* v
spikes. This was done also in this particular installation but, as8 I: H5 C; D; B& j6 S
usual, in the days following the energization the magnet drifted a bit,; D2 e/ C- ]! E/ i1 g
getting closer to the radio station carrier. Furthermore, the usual 13C0 \; @5 ]' K1 X! V
spectral widths are quite wide which makes things even worse. Murphy's% l$ @* m0 y `- J0 Z; \
Law has no exceptions!) } o# p# A8 a4 K6 E
But we are just at the beginning of my real troubles. Before
: t9 {- x- N& ~. P4 f; qputting one's hands on the magnet, one should better know how much, in5 A* n/ A7 s' R9 E& p3 h# i
which direction, should the field be moved. I have therefore used a
0 K+ [7 ~* I) Y: rgood Spectrum Analyzer (Tektronix model 2710) to check the frequency7 }# o# H; U/ [* u4 j" b! e
spectrum around 100 MHz, ready for the worst. And the worst was what I7 |, X' r/ f* P: X4 y$ a# n
got! The band was filled with FM signals, evenly spaced by 250 kHz and. G9 p7 L! J4 K) Z9 T, B
with modulation envelopes as wide as 100 kHz, so that when I got far
( I6 G. a+ o5 ?* m, ]from one station I started receiving the next one; accounting for
! g8 Q0 L2 ~9 M9 q6 P. T. t% hfolding and aliasing effects, there was no chance! The only somewhat% L0 s- V$ p" s. v' Y
free region was at 100,120 MHz, but this implied proton frequency of
) }+ j0 C! v, V) q9 P4 [4 v398.100 MHz. So now the spectrometer is no longer a "400"!
6 z! I* t& i9 o: W" y% w Before installing a spectrometer, you better get a Spectrum
! Q* b; m! I3 d: Z7 |. AAnalyzer and check for the presence of RF fields in the instrument
5 S. n2 `0 Z. b- a& {6 R- z, V8 vroom, taking care to explore the areas close to the observe frequencies5 {% n+ i! u% f
of all the most important nuclei. Don't forget the lock: at 14 T+ y9 W0 J& U$ Z8 s( @7 z
(nominal 1H frequency of 600 MHz) 2H resonates at 92,095 MHz, once
: _5 x( E9 w3 V& {$ oagain in the FM broadcast band. The lock channel receiver has quite
8 r+ e0 Y/ z# U# l& anarrow bandpass filters, so hitting a radio is a really bad luck, but5 k4 R! Z& J1 E; K) O; k+ D
it had already happened, resulting in fast lock level variations and% b8 S( l4 {2 N2 z* i4 `/ A1 M
totally malfunctioning Gradient Shimming which uses deuterium as
( c' X& {' c/ @! N ~, R$ Bobserve nucleus!
4 P1 Z b" u& a: u0 ?( J- [ Needles to say, the extremely high sensitivity of an NMR; t& T; H4 f$ E' X) w7 r- {
Spectrometer shows up. The signal from the guilty radio, as observed on* L2 ]5 i6 u5 G2 p
the spectrum analyzer inside the spectrometer room, had very low% D+ w" H! f W0 z$ S* f
intensity level of about -70 dBm, some microvolt/meter, but that was
$ ~; D% s& ^# Wenough to almost completely hide the quite strong 13C signal from the3 W" w- F9 o8 i1 J
ASTM sample!3 ?8 f( {8 l0 N1 V9 ^( k% a
The radio was clearly picked up by the Probe (closing the
0 q6 E# t; [2 MPreamplifier input with a shielded 50 ohm RF load, all signals
- R2 I- N) B) C3 [% b5 ddisappear) but, quite surprisingly, there is almost no shielding effect+ l; L) D" J) V0 B! p$ z
attributable to the metal body of the magnet, which is after all an7 |, h6 n3 _% y4 \5 h3 r& e. ]
almost completely closed cylinder all around the Probe. Most probably a
- H7 | A3 N R1 p6 Y! ?: s+ `) Ygood deal of the signal leaks in through the Shim Coils which are
f* b/ O" V! y) N; e( k. \mounted very close to the Probe and, together with their connection- b, h& T) Q% [' f& ~& S$ e( n/ r6 J
cables to the Console, constitute a quite good antenna.4 w7 e M+ Y* B) H% T0 M
Too bad the Shim Coils are essential, and effective shielding
+ m( }7 C: k6 [- S0 Z" H* j* |of the instrument with a Faraday's cage is always difficult and
6 n( C3 u9 J$ V: | Z0 T( iexpensive (it may be almost impossible once the spectrometer is
! J$ T' o7 H0 E: F5 n4 |installed).) J$ R5 @( h, w+ y( E+ {
) b& t8 r$ `9 J9 _7 {* s2 {Before concluding, let me venture some additional advice based on my experience:
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= Install the spectrometer in the best shielded room
: s" t' M0 X+ m# Wyou can get; the best choice is once again in the basement, where you8 n6 [- f7 v9 ~6 Z% d8 j& h
have the whole building above the ceiling and its [grounded]
+ I& i9 g% h1 P5 tfoundations all around the rest, done in iron-reinforced concrete," h! ]$ i8 F: t) P0 q
amounting to a good Faraday's cage at no extra cost.
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% ] u6 q9 N# Z7 Z1 Z= If possible, avoid top floors. If you can't avoid- X0 y$ U+ F0 w& `* M: F# h, e
going upstairs, take a good look out of the window: if you see nearby/ s* n# y+ w: ?; N* c9 P
transmission antennas, get ready for troubles proportional to their
8 a4 P7 d0 D% Q7 M# E( A5 Edimensions and closeness (to my knowledge, however, mobile telephony! ?( O7 [) k* ^, T! ]5 o. X
antennas cause so far no harm).' r$ R4 V- s; S5 N
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= I'm sure that an exchange of experiences and/or! C8 n# @ b! ~' g, |- I
suggestions regarding this matter would help a lot to solve many$ M' ^1 x2 Z3 C5 j% f7 j" j
existing installation problems and prevent ones yet to come. Stan's Blog is an ideal location and, needless to say, I will be absolutely glad to cooperate.
% u; i3 A& b2 j5 P, g7 a " E2 u( M4 {% B$ J9 ~8 X) o
Vanni Piccinotti, Firenze, 11 April 2008
摘自stan' NMR Blog.
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