, I; Z& g% S* l6 I( K" `Cross-talk between FM Broadcast Radio Transmitters (88-108 MHz)
# _& j* B/ a6 a- D& i7 t2 t ^and NMR Spectroscopy: A recent experience# Q8 V) V! s, ^: s5 @
9 K) D. t) u9 j9 i4 cRecently I had to install a 400 MHz (9.4 T) NMR Spectrometer. The
; G h, s, ^- Tsystem worked fine and, using an Indirect Detection Probe , met quickly. s, L# ]3 N' t3 g1 m
and effortlessly the specifications. But later on, when the customer
! ?5 p, c& {- R! finstalled a 13C direct detection Probe, the S/N ratio turned out to be+ f- f7 _6 {4 ?% \/ o, l
quite low and, on top of it, the sensitivity was subject to erratic and
6 v. H; T6 [- F5 \very large variations from 50:1 to 130:1 (manufacturer's specs give% g c0 L$ N" R2 J" z+ L( X
155:1), without any apparent reason.
8 y( L# w; V' ^& b; H Since the nominal 13C observe frequency at 9.4 T is 100,568& m4 b( }/ a- E. F; q
MHz, right in the middle of the range of commercial FM broadcasts, I
: D2 }1 w7 i7 t8 K' v6 g5 Ghave immediately suspected that the spectrometer was picking up one of6 g0 e9 D" U: r, N( \$ W
those radio stations. In fact, using a cheap FM radio receiver, a( q% X; @4 i( I+ }
strong station was quickly found at 100,60 MHz. At this point, I have0 i4 R% t; c5 r& ~
connected a simple audio amplifier ending with a loudspeaker to the
9 K* O+ L2 d1 a5 C" noutput BNC of the observe receiver which was there apparently just for9 A/ x$ n/ }- F$ b6 l5 \& B8 |
this purpose, and all of us were listening to the radio using a 200.0008 Z& G. w* w9 j5 U; n; C7 c( V/ f1 q
Euro NMR spectrometer, except that the audio quality was really poor,3 ^' L% d" U3 t( k/ [3 @
much worse than from the above-mentioned gadget radio (a shopping mall! I1 @7 i7 v8 W; w3 g
gift)." K. F# l/ N# f4 A
The problem is well known from the old times, when the highest) i" Q! {+ a& G) L; S Z
field was 2.45 T and the nominal H1 frequency was close to 100 MHz. One* t1 ?- v, F. b& W4 x
of the first Italian NMR spectroscopists to experience it, back in
% Q% ?' i2 ^. r& j* h% s1974, was Prof. L.Lunazzi at University of Bologna, on his brand new
6 P" X; Q: j) M( ~Varian XL100 spectrometer, and the radio station was Radio San Luchino,
- E- ~( B. g; ?2 j6 t' rwell known to anybody living in Bologna, which broadcasts from the top5 d) g5 r& s% t0 K% D
of the nearby Saint Luca hill.
6 U/ A; M0 p, ~% O8 B The obvious solution is to change the magnetic field, and thus
4 p' e/ _1 v+ Fall resonance frequencies, in order to get out of the modulation
% U' L1 W) p- a" }2 Eenvelope of the interfering transmitter. But this is not always easy,4 b0 C: C) Z+ g( w' S2 W
since the range by which one can move the magnetic field changing just& o* f- b% m1 O G
some software parameters is usually limited to a few tens of kHz in the, ?( x7 W5 V% [, t& ~! P
frequency domain. If larger variations are required the poor engineer
3 e8 L0 r0 p! O7 z9 ^3 E' T6 chas to work on the superconducting coils of the magnet, which is a- c6 a7 P9 y0 F
no-trivial job entailing the risk of a total or partial quench.
, N* h/ \6 ?6 {. y, j Bitter experience shows that persuading the involved radio
5 k$ p; Y k! [% ^9 `- [. jstation to change its operating frequency is a time consuming,7 v7 m. X) c7 y2 o2 s: m0 p* E/ t
frustrating, and apparently quite impossible task.
! E/ l) _9 ~# y+ c Being well aware of the problem, my preliminary spectrometer
+ C. i4 P& [ R4 |2 zchecks always include some blank acquisitions taken before running up+ m4 V$ a' P( z( v0 x
the magnet so that there is no chance to observe an NMR signal. The
1 J2 p7 ~( M* r7 j- D R6 b7 ~resulting dataset should be pure white noise, without significant
4 i5 I3 \, n8 p. P/ |8 tspikes. This was done also in this particular installation but, as
- }, R; X" _" h% p" S( j5 yusual, in the days following the energization the magnet drifted a bit,
; }" A& B6 w, z& @6 ?" \getting closer to the radio station carrier. Furthermore, the usual 13C
1 c# J& c8 j' y! dspectral widths are quite wide which makes things even worse. Murphy's! H- S$ C. _0 O0 ?
Law has no exceptions!, E& Y! [! s# x, L e
But we are just at the beginning of my real troubles. Before
6 r+ S6 |; d4 A3 Y$ T5 xputting one's hands on the magnet, one should better know how much, in% z) r$ E3 P, }$ f* y: j9 L; _
which direction, should the field be moved. I have therefore used a
- Y) g7 |$ H4 D( W8 zgood Spectrum Analyzer (Tektronix model 2710) to check the frequency( a' E% F% a! ~
spectrum around 100 MHz, ready for the worst. And the worst was what I+ Y0 V+ ^# m9 {6 @6 z2 H
got! The band was filled with FM signals, evenly spaced by 250 kHz and
" k0 ~# t/ Y* z2 Y7 F1 Cwith modulation envelopes as wide as 100 kHz, so that when I got far: E" T- m: S5 U" X1 k- T
from one station I started receiving the next one; accounting for& m3 x/ g' y; F. i" w3 N4 j3 C
folding and aliasing effects, there was no chance! The only somewhat
( X! z& g" n4 i( v. xfree region was at 100,120 MHz, but this implied proton frequency of
- a, u! i {: {1 z. H' s8 U398.100 MHz. So now the spectrometer is no longer a "400"!% r+ g5 a7 g% ] m) X. N9 H* e6 ?
Before installing a spectrometer, you better get a Spectrum
6 T2 S$ l% Z2 ~2 u4 AAnalyzer and check for the presence of RF fields in the instrument
6 n# ]3 a/ C) f& ^$ q& |room, taking care to explore the areas close to the observe frequencies% w$ P- j: n6 t( }& L! y
of all the most important nuclei. Don't forget the lock: at 14 T
) S( @% j0 |" ?$ B. C/ r. b(nominal 1H frequency of 600 MHz) 2H resonates at 92,095 MHz, once
( a, u5 z( R7 Y) Nagain in the FM broadcast band. The lock channel receiver has quite
3 }& B2 m" w- U$ _5 N vnarrow bandpass filters, so hitting a radio is a really bad luck, but
6 ] P( e5 @7 k) w# o$ ?it had already happened, resulting in fast lock level variations and
, a+ `7 s$ r* o5 T/ d" }& rtotally malfunctioning Gradient Shimming which uses deuterium as; W8 I5 P( A8 O7 h4 g/ W- m
observe nucleus!' Q' }" i# c. H/ R3 i- B0 ^
Needles to say, the extremely high sensitivity of an NMR
% M1 i' J' l8 e2 ^0 KSpectrometer shows up. The signal from the guilty radio, as observed on
3 N+ V; U& P. j7 f" ythe spectrum analyzer inside the spectrometer room, had very low
- G! Q; Z7 U. f) {1 T# \intensity level of about -70 dBm, some microvolt/meter, but that was
: ^1 M4 S( }) i# `8 ?enough to almost completely hide the quite strong 13C signal from the
: m: n8 B1 `1 D. [& C( LASTM sample!* j( ~4 A. H. r
The radio was clearly picked up by the Probe (closing the v1 T: U+ Z+ S6 @. q- }( `
Preamplifier input with a shielded 50 ohm RF load, all signals+ ?7 U1 m2 j* O( H
disappear) but, quite surprisingly, there is almost no shielding effect
) Z. s) K5 [( oattributable to the metal body of the magnet, which is after all an
) i& Y/ v8 D0 m1 a) c3 R9 }# zalmost completely closed cylinder all around the Probe. Most probably a3 k6 _) V6 s3 q+ P/ U- r
good deal of the signal leaks in through the Shim Coils which are6 L3 g" J: x9 J3 Q
mounted very close to the Probe and, together with their connection
% {. n- T+ Y2 F1 I' u# F9 zcables to the Console, constitute a quite good antenna.
7 [0 M2 L% K4 ~6 ]5 h% ~ Too bad the Shim Coils are essential, and effective shielding! y- J+ A3 k0 v
of the instrument with a Faraday's cage is always difficult and0 @, H. B7 @1 T) k2 Z" k8 H
expensive (it may be almost impossible once the spectrometer is
) Q' o' Q5 R7 A& _' |" G$ F2 ~installed).8 c( O. ~* ]! B$ c+ |" Q) W9 u
- k" X: c2 o: }4 ?- A
Before concluding, let me venture some additional advice based on my experience:: r$ y# O) E% A6 }- A8 Y, y
' _" p9 S3 l" a& ?/ U
= Install the spectrometer in the best shielded room
$ T2 y6 U$ O4 n0 M: X1 D; E6 `5 lyou can get; the best choice is once again in the basement, where you% D3 V5 }( @, q; C
have the whole building above the ceiling and its [grounded]4 W' Y/ z6 s) t$ x7 K) N7 e/ j$ ?: u
foundations all around the rest, done in iron-reinforced concrete,
* h+ Q1 Q. K; |+ l1 L! {/ t9 tamounting to a good Faraday's cage at no extra cost.0 p& p5 M! Z( I- C: p( U6 m
/ }" N+ [% X: G; u3 @5 O6 n% y
= If possible, avoid top floors. If you can't avoid
" Q# |" F: c4 D \' Qgoing upstairs, take a good look out of the window: if you see nearby2 g+ M# s+ l) B! p7 \. i! W+ Y5 \
transmission antennas, get ready for troubles proportional to their6 S$ v5 X/ Z5 | M
dimensions and closeness (to my knowledge, however, mobile telephony
1 _% ~. r2 E! [& c5 G H7 {7 wantennas cause so far no harm).& r7 ^& w' g, v. ?( z( x
$ M0 c- V+ ?" Z5 r6 _' |
= I'm sure that an exchange of experiences and/or$ N: |" ~1 P" a9 D+ C: y/ E6 @
suggestions regarding this matter would help a lot to solve many, w; X) T, T q
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.
& D" A% {9 [+ a6 L/ C2 v
c: M: X( o% QVanni Piccinotti, Firenze, 11 April 2008
摘自stan' NMR Blog.
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