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Cross-talk between FM Broadcast Radio Transmitters (88-108 MHz)
2 O0 W$ G, J5 b9 x4 ^0 t+ jand NMR Spectroscopy: A recent experience9 w8 M- O- Z0 S5 U. g* W
t1 o8 J( A1 y
Recently I had to install a 400 MHz (9.4 T) NMR Spectrometer. The
) w# `7 F# v! S8 v7 t. J, m2 d. Qsystem worked fine and, using an Indirect Detection Probe , met quickly' r S3 g( Y- U j1 `* ^3 @
and effortlessly the specifications. But later on, when the customer
: J1 I/ M4 \ R5 {' Kinstalled a 13C direct detection Probe, the S/N ratio turned out to be5 B$ `7 C% O& o, {7 R! q+ ]
quite low and, on top of it, the sensitivity was subject to erratic and% d5 J- ]3 g; H! H
very large variations from 50:1 to 130:1 (manufacturer's specs give6 S7 j( y& H9 g$ A; V
155:1), without any apparent reason.
, W4 ]1 P! V/ N3 ~$ l* e# Y# q Since the nominal 13C observe frequency at 9.4 T is 100,568
& ]% z2 B. Y" b1 u/ gMHz, right in the middle of the range of commercial FM broadcasts, I
3 k9 |+ c. R' @7 `8 ~8 jhave immediately suspected that the spectrometer was picking up one of
% u$ N$ j, f5 K; O7 X% a+ h$ P9 hthose radio stations. In fact, using a cheap FM radio receiver, a
, P: E5 I7 D6 q) M1 ustrong station was quickly found at 100,60 MHz. At this point, I have
2 w1 }. h6 @" X! P* Iconnected a simple audio amplifier ending with a loudspeaker to the( w4 K4 L3 |5 N4 q) z2 m7 Z4 ^
output BNC of the observe receiver which was there apparently just for
3 P" {6 B+ y D% b, T- hthis purpose, and all of us were listening to the radio using a 200.000' y2 [1 x; O% ^) h. e
Euro NMR spectrometer, except that the audio quality was really poor,, t- B0 Q) D6 p$ s+ n4 s
much worse than from the above-mentioned gadget radio (a shopping mall4 \2 A7 Z8 _) N8 n" N& c
gift).2 _3 W; h( |4 q, U
The problem is well known from the old times, when the highest) G& B r s3 r7 x( L) F# ]
field was 2.45 T and the nominal H1 frequency was close to 100 MHz. One! [/ U, p8 w# t: A7 w5 X) O
of the first Italian NMR spectroscopists to experience it, back in+ P1 ~4 \7 z3 e5 Y. I
1974, was Prof. L.Lunazzi at University of Bologna, on his brand new
2 \+ a7 q0 d/ a$ A* c! NVarian XL100 spectrometer, and the radio station was Radio San Luchino,! K0 |% V+ A: m' o! i
well known to anybody living in Bologna, which broadcasts from the top
7 Y& [/ H$ {, {6 I; w1 e' t+ lof the nearby Saint Luca hill.
- J( I! Q( S0 V% w6 Z/ m! m. q" ? The obvious solution is to change the magnetic field, and thus& z0 L! T" ]& [( e# G3 T5 L6 B
all resonance frequencies, in order to get out of the modulation) l( Z, n$ \# s( q
envelope of the interfering transmitter. But this is not always easy,
/ F& F# A' f! e/ A6 y$ \since the range by which one can move the magnetic field changing just
5 p: ^4 r8 w$ ^/ h# gsome software parameters is usually limited to a few tens of kHz in the
( K3 A9 e/ O* g8 H' Cfrequency domain. If larger variations are required the poor engineer
- F0 p% w# G" R8 F3 D" Vhas to work on the superconducting coils of the magnet, which is a
# a4 Y+ {9 Q+ {$ w/ S- x% ono-trivial job entailing the risk of a total or partial quench.8 j4 q) R. b z3 Q1 _" @, m) c
Bitter experience shows that persuading the involved radio# n3 W% z5 I( a! M# L9 M
station to change its operating frequency is a time consuming,% S4 l7 k7 W; ~9 t2 v8 U& l
frustrating, and apparently quite impossible task.# L$ }! P$ f' \2 \
Being well aware of the problem, my preliminary spectrometer
( Y6 O( z* R2 g* K2 w, E- T) Fchecks always include some blank acquisitions taken before running up
/ i$ ^8 `3 j- P( E9 Bthe magnet so that there is no chance to observe an NMR signal. The' q! p6 x+ r3 \ }; G
resulting dataset should be pure white noise, without significant: u- D0 e: n: n' s6 w. M
spikes. This was done also in this particular installation but, as
3 w) U/ x- y9 L# Eusual, in the days following the energization the magnet drifted a bit,
^$ K/ P' l, F0 f! W- D3 Dgetting closer to the radio station carrier. Furthermore, the usual 13C! h- j) T" z4 `1 o) D/ B' ?
spectral widths are quite wide which makes things even worse. Murphy's
* k+ h! T+ k" l) y& t- d; YLaw has no exceptions!; s! r( ^# \- h9 G z
But we are just at the beginning of my real troubles. Before
0 f9 y2 `; N7 E# E z8 O' d( Nputting one's hands on the magnet, one should better know how much, in
$ ~3 L; U3 P& }( F+ v; P1 C0 Owhich direction, should the field be moved. I have therefore used a
( ^) i; q5 G: Ngood Spectrum Analyzer (Tektronix model 2710) to check the frequency
) G" `2 s9 u( Z2 G# }0 T6 U) \spectrum around 100 MHz, ready for the worst. And the worst was what I
# x4 _/ A. s; E. d2 n, O0 {7 Hgot! The band was filled with FM signals, evenly spaced by 250 kHz and
" V: m, a9 n+ k) c) Qwith modulation envelopes as wide as 100 kHz, so that when I got far" s3 T5 R$ F1 {- h( t- l# L
from one station I started receiving the next one; accounting for
3 Z. `0 O! v$ H8 F4 T, lfolding and aliasing effects, there was no chance! The only somewhat
2 B2 ~5 g1 C" q: X) M$ w- hfree region was at 100,120 MHz, but this implied proton frequency of) s& u& {$ q5 R+ c! l3 g
398.100 MHz. So now the spectrometer is no longer a "400"!
2 O% I( n* p+ D+ F4 B+ k! z' F+ c Before installing a spectrometer, you better get a Spectrum3 ]* A: E' N, }- ^9 F
Analyzer and check for the presence of RF fields in the instrument4 X! _, T3 t v T
room, taking care to explore the areas close to the observe frequencies7 P+ c- N! ?5 J( g7 n
of all the most important nuclei. Don't forget the lock: at 14 T
: z2 n# [) u2 q$ O5 @(nominal 1H frequency of 600 MHz) 2H resonates at 92,095 MHz, once
1 ]! T' ^1 i1 o$ W+ x2 lagain in the FM broadcast band. The lock channel receiver has quite- E! ^( ^! g& L4 i+ r
narrow bandpass filters, so hitting a radio is a really bad luck, but* k7 e" @1 [$ J7 L, I; f
it had already happened, resulting in fast lock level variations and
* |1 e0 x2 u4 rtotally malfunctioning Gradient Shimming which uses deuterium as
: k( y7 P$ ^7 ]observe nucleus!
0 b1 W( u9 |+ m Needles to say, the extremely high sensitivity of an NMR, _( D& [& s0 ~( W7 T. |
Spectrometer shows up. The signal from the guilty radio, as observed on
6 \. O) I- q- [; G+ c: \0 x; c+ R+ Z! Dthe spectrum analyzer inside the spectrometer room, had very low
0 d/ ^! k7 Y; [1 mintensity level of about -70 dBm, some microvolt/meter, but that was
# _( P! I2 g- @) W7 D/ Menough to almost completely hide the quite strong 13C signal from the! Y7 J; t- _7 f: R5 C$ B. z( y
ASTM sample!
7 U5 q7 M* ]. ?9 n C The radio was clearly picked up by the Probe (closing the
2 o( ~0 Z* u+ V3 ]# F3 CPreamplifier input with a shielded 50 ohm RF load, all signals V6 P! b3 y3 E4 N8 a
disappear) but, quite surprisingly, there is almost no shielding effect
$ \% K# R) G, ~" Aattributable to the metal body of the magnet, which is after all an
% _* ^; L: u, P9 x9 valmost completely closed cylinder all around the Probe. Most probably a
+ l ]/ K2 y6 b% pgood deal of the signal leaks in through the Shim Coils which are
* u( X3 C, O4 }' t+ x+ i6 C& jmounted very close to the Probe and, together with their connection
( U/ C. S; j4 q+ i1 ~( G/ U& U, Z2 }cables to the Console, constitute a quite good antenna.. A& m9 B( G \* U( ^: o0 o
Too bad the Shim Coils are essential, and effective shielding
9 @+ h# q) ~+ qof the instrument with a Faraday's cage is always difficult and; I7 @( j$ Q" y* Q1 c* _
expensive (it may be almost impossible once the spectrometer is
( B! V: c/ v5 [% X6 p4 @; Y2 Z/ ?+ pinstalled).8 q2 |0 L$ M8 U7 [9 r
! n/ i: D. y7 |7 v( gBefore concluding, let me venture some additional advice based on my experience:
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/ y* P! q' H1 F' S( _= Install the spectrometer in the best shielded room1 Y2 O" ?( N3 {) _
you can get; the best choice is once again in the basement, where you
5 s$ U8 K3 S) O* |5 Z$ Khave the whole building above the ceiling and its [grounded]6 l9 @$ x/ K b4 x; l* [
foundations all around the rest, done in iron-reinforced concrete,
7 m4 i7 I$ o% z2 `) E+ s3 x4 vamounting to a good Faraday's cage at no extra cost.
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= If possible, avoid top floors. If you can't avoid
6 ?$ B8 m; ?& w. y; h$ A( fgoing upstairs, take a good look out of the window: if you see nearby
* S5 T" o. l u; {+ J( y1 p9 ftransmission antennas, get ready for troubles proportional to their
9 {8 I8 ?' E% L0 Odimensions and closeness (to my knowledge, however, mobile telephony
3 ~' B3 s$ [" r% B) n9 ~antennas cause so far no harm).
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) F- `- g- K0 P= I'm sure that an exchange of experiences and/or. Q; ]: n* l0 q* r! T
suggestions regarding this matter would help a lot to solve many
4 ]# x* m) M: }$ {% x) X, oexisting 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.
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% E# j" T* Q$ w+ Z4 gVanni Piccinotti, Firenze, 11 April 2008
摘自stan' NMR Blog.
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