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" N* L z9 a! GCross-talk between FM Broadcast Radio Transmitters (88-108 MHz)5 Y" B# s( }- Y, r2 [1 @. @
and NMR Spectroscopy: A recent experience, j, s- i+ z" F" i% I ?/ M
/ ], e6 q, }4 N( ]Recently I had to install a 400 MHz (9.4 T) NMR Spectrometer. The
; }; W9 A u$ fsystem worked fine and, using an Indirect Detection Probe , met quickly
1 z4 V, P$ P- r2 Z6 S: Oand effortlessly the specifications. But later on, when the customer. c8 \+ a1 Q/ @0 X
installed a 13C direct detection Probe, the S/N ratio turned out to be
3 q* u. i* j0 xquite low and, on top of it, the sensitivity was subject to erratic and& c6 c" g0 g* G! v1 l
very large variations from 50:1 to 130:1 (manufacturer's specs give
7 \8 U& L% F% k6 I1 O# U X155:1), without any apparent reason.
6 r3 s% ^1 C; C" u4 I' [ Since the nominal 13C observe frequency at 9.4 T is 100,568
# r, N- M# g# p. |MHz, right in the middle of the range of commercial FM broadcasts, I. O6 Z/ T7 d3 u" h6 L2 p
have immediately suspected that the spectrometer was picking up one of
$ y1 F% P. k; u7 Y& E% L3 Zthose radio stations. In fact, using a cheap FM radio receiver, a
% L$ \- S! J. E, u/ Fstrong station was quickly found at 100,60 MHz. At this point, I have
( D: a- ?7 z2 J2 ^4 F6 `connected a simple audio amplifier ending with a loudspeaker to the. Q6 p P5 a( ?1 F" e: z$ Y
output BNC of the observe receiver which was there apparently just for! s" n0 K- Y' _- `% J
this purpose, and all of us were listening to the radio using a 200.000
' k% g! x" ~3 }" }$ C) _+ h5 ~9 AEuro NMR spectrometer, except that the audio quality was really poor, u! U. t, Q \' v* n
much worse than from the above-mentioned gadget radio (a shopping mall$ h: M4 T5 G7 S# r- C. a0 a9 W! S
gift).8 p0 I$ B$ H: i6 s0 M2 V
The problem is well known from the old times, when the highest
3 C$ f R6 b% w3 N. e- a ?% Bfield was 2.45 T and the nominal H1 frequency was close to 100 MHz. One
9 n, I7 B9 F2 S( P; G. ]7 Vof the first Italian NMR spectroscopists to experience it, back in, J) |7 A' ~* s( R
1974, was Prof. L.Lunazzi at University of Bologna, on his brand new: i. v2 }% }& [- B! u9 \
Varian XL100 spectrometer, and the radio station was Radio San Luchino,6 u, m( Y: w J6 W- f+ L
well known to anybody living in Bologna, which broadcasts from the top
) a; ~( s1 |; a- B) `- A8 O0 zof the nearby Saint Luca hill.
9 Y* ~7 S5 l) B The obvious solution is to change the magnetic field, and thus+ p4 W7 ^& l( ?) ~5 ]2 n
all resonance frequencies, in order to get out of the modulation
) \6 b0 R0 B+ ]envelope of the interfering transmitter. But this is not always easy,
6 s3 A, i& j6 Z0 I! N$ H$ R( C3 Gsince the range by which one can move the magnetic field changing just
" l& U# t( u% _4 Hsome software parameters is usually limited to a few tens of kHz in the% m! m! g- Y6 v( @8 B
frequency domain. If larger variations are required the poor engineer
2 j0 R* g5 W ~$ w0 Dhas to work on the superconducting coils of the magnet, which is a/ I/ D6 g: u. ^" U t d" P9 I
no-trivial job entailing the risk of a total or partial quench.
9 } P! o8 p/ j! v8 P Bitter experience shows that persuading the involved radio" V. a0 s! ?' B
station to change its operating frequency is a time consuming,3 o: C; Q* x1 G0 F6 n. u7 C
frustrating, and apparently quite impossible task.3 m) a( u& }3 T
Being well aware of the problem, my preliminary spectrometer' ?7 S1 O) m8 W M G9 V
checks always include some blank acquisitions taken before running up4 ^$ j: T( Y6 q: l( C
the magnet so that there is no chance to observe an NMR signal. The
( |/ G4 m. R1 }' a% [resulting dataset should be pure white noise, without significant
& F' B3 l$ O, ]) q I% ?spikes. This was done also in this particular installation but, as! P' Y, S/ Z4 U. A
usual, in the days following the energization the magnet drifted a bit,+ Q: ?; x5 {- }& U% |
getting closer to the radio station carrier. Furthermore, the usual 13C8 R7 l2 v' \) A$ d: s% ~ _
spectral widths are quite wide which makes things even worse. Murphy's1 m0 I4 u0 N2 g2 i, O3 |. ?+ T
Law has no exceptions!
6 }4 s; r% w1 M But we are just at the beginning of my real troubles. Before
. p% L% l8 m7 T4 ^3 Z7 \putting one's hands on the magnet, one should better know how much, in4 m3 T9 H$ `. m2 l( E3 _8 e4 e3 t
which direction, should the field be moved. I have therefore used a- b) ?5 r4 T% p/ R4 |# h/ q
good Spectrum Analyzer (Tektronix model 2710) to check the frequency, [. K$ v2 A# D: ^/ y
spectrum around 100 MHz, ready for the worst. And the worst was what I
) ^8 R) t/ b2 ygot! The band was filled with FM signals, evenly spaced by 250 kHz and
% M4 \+ l5 Q, nwith modulation envelopes as wide as 100 kHz, so that when I got far
/ i5 }# z7 }. k# Lfrom one station I started receiving the next one; accounting for
" k# d' S i0 s( s0 [folding and aliasing effects, there was no chance! The only somewhat' N* m! m6 f7 J
free region was at 100,120 MHz, but this implied proton frequency of
0 @/ `/ j- F+ o398.100 MHz. So now the spectrometer is no longer a "400"!. Q- x3 L- u( f& ? G5 I
Before installing a spectrometer, you better get a Spectrum$ e5 O% U) K$ {' g, U. s
Analyzer and check for the presence of RF fields in the instrument. W/ c- \, A2 \0 W) Y. r3 M
room, taking care to explore the areas close to the observe frequencies( z$ C: r, J! I
of all the most important nuclei. Don't forget the lock: at 14 T0 w( {$ p4 {) h9 u/ M( ]
(nominal 1H frequency of 600 MHz) 2H resonates at 92,095 MHz, once
" ?( S+ B* c6 g g- ~8 l+ Fagain in the FM broadcast band. The lock channel receiver has quite1 D I- E* z* A5 a5 c% J. ?, {
narrow bandpass filters, so hitting a radio is a really bad luck, but0 b& U6 ?: O6 D) M0 E. o( F) e
it had already happened, resulting in fast lock level variations and' |5 r# \3 u; i9 U4 I
totally malfunctioning Gradient Shimming which uses deuterium as
) J5 m; H4 f6 n' h, Mobserve nucleus!
% [5 `0 k9 v2 c8 }, e3 [# \1 T Needles to say, the extremely high sensitivity of an NMR" Q8 K9 ]2 Q. a* h: r3 ]
Spectrometer shows up. The signal from the guilty radio, as observed on( J( w& z# @% g7 X) ]& `2 Q
the spectrum analyzer inside the spectrometer room, had very low9 z F* x& `3 x3 W
intensity level of about -70 dBm, some microvolt/meter, but that was
) w G% T" }2 h" k) ~enough to almost completely hide the quite strong 13C signal from the, E' ~/ }7 p4 |! q# V$ ]' E9 M% ?6 S4 F
ASTM sample!
6 l* ?, E: @6 _* Y* S The radio was clearly picked up by the Probe (closing the0 @& L7 h# E& a- l! M
Preamplifier input with a shielded 50 ohm RF load, all signals4 n* g7 F8 P! [5 a A& |) r' L
disappear) but, quite surprisingly, there is almost no shielding effect
: B i, V' T0 z1 M3 h2 `attributable to the metal body of the magnet, which is after all an
: G; V- d& C, Z! s5 s9 Falmost completely closed cylinder all around the Probe. Most probably a" Y- Z9 d/ c1 e7 a- b( t
good deal of the signal leaks in through the Shim Coils which are7 f3 @. }& k. q5 L H0 h
mounted very close to the Probe and, together with their connection7 a( T" B8 V4 q) a
cables to the Console, constitute a quite good antenna.& E% s; \8 T" W1 k. m3 |8 Q
Too bad the Shim Coils are essential, and effective shielding
$ _5 A/ N. x* z4 Q& {/ D6 wof the instrument with a Faraday's cage is always difficult and) s9 L) P: m3 D' W2 F" |( _
expensive (it may be almost impossible once the spectrometer is# ?( e* A( i/ q, O! T, o4 r0 A$ b
installed).
4 F# W# D; m) M- h
: @4 {; _' S8 `) A1 ]Before concluding, let me venture some additional advice based on my experience:1 @) h9 J# Z! D/ V" W/ u) w* ~; o
v+ ~. [7 f1 b
= Install the spectrometer in the best shielded room
2 W' a7 S1 f4 e8 K0 Z4 lyou can get; the best choice is once again in the basement, where you
9 n/ d& q# ?) Phave the whole building above the ceiling and its [grounded]
8 v( i: [& k% f. |! T3 z! sfoundations all around the rest, done in iron-reinforced concrete,5 t9 ]5 B! Q5 k8 d/ w2 l8 Z2 R" ]
amounting to a good Faraday's cage at no extra cost.
5 e3 n7 N' i' q2 i; g* v3 }
) U7 @5 F: Z; o0 u= If possible, avoid top floors. If you can't avoid& d4 C1 L* o Z1 l3 B
going upstairs, take a good look out of the window: if you see nearby, J( J8 `; f- \8 z
transmission antennas, get ready for troubles proportional to their% r7 q. W1 A7 Y: f3 S+ N7 U n
dimensions and closeness (to my knowledge, however, mobile telephony
" u9 Z7 g4 P$ {! y2 R7 santennas cause so far no harm).( o W5 O" N2 A( I2 d, J' q+ G
" _3 J7 ^" g9 y= I'm sure that an exchange of experiences and/or1 c7 I) S5 {4 a9 {
suggestions regarding this matter would help a lot to solve many7 L+ v3 R2 c2 I0 E* Z8 T
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.% D7 O. S% v5 K
4 ^" E3 Z: i+ ]* X8 ?/ hVanni Piccinotti, Firenze, 11 April 2008
摘自stan' NMR Blog.
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