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无线电台会影响NMR

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发表于 2008-7-1 02:51:48 | 显示全部楼层 |阅读模式
 When it comes to polluting the environment, humanity has no equals.& l% @1 u( @0 n* N: ^/ d This applies to all kinds of spaces, including the electromagnetic' t" m7 L c, c ether. What follows is a contribution and a warning from Vanni Piccinotti,3 o' q# b9 _) |( V: G+ m! j5 O# l an engineer based in Florence, Italy, who has decades of experience# z: @/ [% P/ W8 {7 n; z6 i with installing, testing, and servicing NMR and EPR spectrometers. The ! Q: w; v3 V2 O0 X& I2 n- Zproblem of RF interference has never been trivial and it keeps slowly + v7 ]" V# v1 j9 x$ zbut inexorably mounting. The spread of urban areas (combined with the- L( q8 R$ f( X: O* X tendency to install MR instruments in those same areas) and the9 G8 U3 q9 Q' C& V' a mounting maze of wireless technologies penetrating our daily life spell4 L2 E0 `! \7 }6 D* Y nothing good for the future quality of our NMR signals. With concurrent 5 {$ u) n' @$ _0 ^. G( kprogress in basic sensitivity of the instruments, time might come when . d k; c2 t- i1 `$ tenvironmental RF noise will be the single major obstacle to further 3 ^# k8 V- b+ V! k% H7 aprogress. But let us hear what Vanni has to say:
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 楼主| 发表于 2008-7-1 02:53:56 | 显示全部楼层
 

, e& Y* E# X5 j& |! D4 |+ a. J( f+ g Cross-talk between FM Broadcast Radio Transmitters (88-108 MHz)1 F. D5 S* @! R* E$ W0 B" |0 `) { and NMR Spectroscopy: A recent experience) z, G) u ]0 P& }

7 v) }) n& M( \/ d+ bRecently I had to install a 400 MHz (9.4 T) NMR Spectrometer. The : {8 J+ a! Q* f1 d. usystem worked fine and, using an Indirect Detection Probe , met quickly9 r* }6 \, E, X! h and effortlessly the specifications. But later on, when the customer2 ?3 U4 i) T d" { installed a 13C direct detection Probe, the S/N ratio turned out to be , v- Q0 \5 w7 j4 H, w% p/ oquite low and, on top of it, the sensitivity was subject to erratic and i4 L4 v% F! o; Y4 i very large variations from 50:1 to 130:1 (manufacturer's specs give . ^) o4 ]6 K: Z( C155:1), without any apparent reason.& E( P, q5 S+ W7 s8 v: y4 |

Since the nominal 13C observe frequency at 9.4 T is 100,568 ( S/ c, H/ H( m: Y. H9 Y2 {MHz, right in the middle of the range of commercial FM broadcasts, I 4 I9 Z9 o/ y0 Fhave immediately suspected that the spectrometer was picking up one of & A$ i% D4 l0 Kthose radio stations. In fact, using a cheap FM radio receiver, a$ I; t, }" ~" D& [& W strong station was quickly found at 100,60 MHz. At this point, I have 1 V! |2 H; L1 }connected a simple audio amplifier ending with a loudspeaker to the 8 ^/ D0 G+ B* U" V9 joutput BNC of the observe receiver which was there apparently just for6 f1 x+ y# q1 r4 Z this purpose, and all of us were listening to the radio using a 200.0004 q* X, W0 j. B Y: ~2 W& l Euro NMR spectrometer, except that the audio quality was really poor,# j3 T/ \ c, a5 J. g* ^ much worse than from the above-mentioned gadget radio (a shopping mall6 S+ E7 @0 h3 B5 l* D3 n7 g; \ gift).3 C0 d4 H) l0 q- M3 _: N

The problem is well known from the old times, when the highest : ], z% a7 W4 T: f# S5 `6 ~field was 2.45 T and the nominal H1 frequency was close to 100 MHz. One / z. O+ Z9 j. y% I( ?( ~of the first Italian NMR spectroscopists to experience it, back in ( h4 p6 w( Q' O- ^' K( b6 Y' s) F1 k1974, was Prof. L.Lunazzi at University of Bologna, on his brand new! Z# d# w. x# I1 j& Z% x9 O Varian XL100 spectrometer, and the radio station was Radio San Luchino, ( m) T0 p9 Q4 cwell known to anybody living in Bologna, which broadcasts from the top : L. r( H# \6 {0 J0 @& \of the nearby Saint Luca hill.. N7 w) [0 }; E* `9 o' ~# G5 h' w

The obvious solution is to change the magnetic field, and thus% o7 K% m( Q1 \ all resonance frequencies, in order to get out of the modulation8 f) e7 a0 z: B% z( g envelope of the interfering transmitter. But this is not always easy,) x: c# o$ `# y8 [' o since the range by which one can move the magnetic field changing just * O: F# ~6 s8 @, [$ rsome software parameters is usually limited to a few tens of kHz in the' z) v! z) y1 r3 r* g frequency domain. If larger variations are required the poor engineer9 O% O( ^, f1 Q | has to work on the superconducting coils of the magnet, which is a : n* F5 y# b c1 K9 mno-trivial job entailing the risk of a total or partial quench.* U/ n4 V" W& j5 @

Bitter experience shows that persuading the involved radio; v4 Y) M$ b* F& F1 w; x6 a' h G station to change its operating frequency is a time consuming, ' M2 a" h; j3 l& \frustrating, and apparently quite impossible task. 6 G8 A) I' q+ N" y) m3 y+ m

Being well aware of the problem, my preliminary spectrometer$ D; Q' b& S g2 i$ L& @ checks always include some blank acquisitions taken before running up5 h- I; j; G2 ?, w- H% x the magnet so that there is no chance to observe an NMR signal. The% s. U4 j2 e" x7 O/ Q resulting dataset should be pure white noise, without significant, t9 r* ~/ w% |7 e2 d spikes. This was done also in this particular installation but, as, n- n1 C# @' {: m usual, in the days following the energization the magnet drifted a bit, ) ~; I$ U: `2 Y1 r) kgetting closer to the radio station carrier. Furthermore, the usual 13C' t7 v& [: ` ^% g$ s: F1 M8 L spectral widths are quite wide which makes things even worse. Murphy's6 e) i9 J0 P' l, @4 E' h' Z0 a4 d8 G Law has no exceptions! 9 ]1 t8 j9 q; k8 y3 w, \+ R

But we are just at the beginning of my real troubles. Before 4 r7 P9 W; r* `putting one's hands on the magnet, one should better know how much, in/ x6 t% B; U4 R+ P2 v which direction, should the field be moved. I have therefore used a Y- f Y) i Y: Y" {, v good Spectrum Analyzer (Tektronix model 2710) to check the frequency $ f3 b$ z/ z4 l) l+ z% A' X. B" dspectrum around 100 MHz, ready for the worst. And the worst was what I" J% [9 x H" |3 c& @0 b got! The band was filled with FM signals, evenly spaced by 250 kHz and7 K* c( u1 p" F2 R with modulation envelopes as wide as 100 kHz, so that when I got far5 W$ ~! @* B: w3 I4 C: _( k from one station I started receiving the next one; accounting for 4 ^% l: z; z2 K1 L$ E' ~ ^folding and aliasing effects, there was no chance! The only somewhat 2 y" J" G. C$ W: g X2 n3 Q, Ofree region was at 100,120 MHz, but this implied proton frequency of . r0 s z: T. Q9 S+ Z" G398.100 MHz. So now the spectrometer is no longer a "400"! ( O! |- d8 L# z! V

Before installing a spectrometer, you better get a Spectrum I' i: d' `' U% w1 P5 |Analyzer and check for the presence of RF fields in the instrument) |# m, ~8 t9 g) f- ?# ? room, taking care to explore the areas close to the observe frequencies# T7 o; K8 G& X2 t% s4 G of all the most important nuclei. Don't forget the lock: at 14 T4 k1 K( D) S- O) }- c (nominal 1H frequency of 600 MHz) 2H resonates at 92,095 MHz, once % T5 q- j1 y" g* }4 Jagain in the FM broadcast band. The lock channel receiver has quite* y5 r, m" Y$ [" E narrow bandpass filters, so hitting a radio is a really bad luck, but2 r) T( _; c! B" X8 F. _ it had already happened, resulting in fast lock level variations and * b2 ]; |: J+ l* ttotally malfunctioning Gradient Shimming which uses deuterium as 6 P! C. p/ c* M0 C- Fobserve nucleus!( X0 |% L/ K8 u0 ]* `

Needles to say, the extremely high sensitivity of an NMR' Z$ O8 m: _" E; }. |3 ? Spectrometer shows up. The signal from the guilty radio, as observed on ! Z) R+ u" l+ L7 |3 ^. l) o* Bthe spectrum analyzer inside the spectrometer room, had very low / T) h, ?. v3 j% F( x( u0 bintensity level of about -70 dBm, some microvolt/meter, but that was( X6 z* ~6 K; n# e" ^ ] enough to almost completely hide the quite strong 13C signal from the 4 a9 ?$ J/ g. A' U6 zASTM sample!. {! r3 b# B% s0 L; p) Q

The radio was clearly picked up by the Probe (closing the, U- c" {1 d7 d- I1 x0 U Preamplifier input with a shielded 50 ohm RF load, all signals 4 C) o# ^* N7 P" D% udisappear) but, quite surprisingly, there is almost no shielding effect ! S: x' K' t& t" t+ tattributable to the metal body of the magnet, which is after all an1 k! f+ ^2 h5 `7 @ almost completely closed cylinder all around the Probe. Most probably a : N. G# W! d$ B3 O2 bgood deal of the signal leaks in through the Shim Coils which are 0 Z5 c- i: A8 X% Rmounted very close to the Probe and, together with their connection E' y, b2 ?2 V) W2 p/ R$ k/ Q) R cables to the Console, constitute a quite good antenna.& {' q& E$ r, S, x: D

Too bad the Shim Coils are essential, and effective shielding$ }' {2 T' d8 }8 Y of the instrument with a Faraday's cage is always difficult and8 T' A2 L# k9 r6 x c7 P expensive (it may be almost impossible once the spectrometer is* K6 D, i2 P# _1 Q& H+ [ installed).! U/ P* O7 D, A- T

7 G& Y7 m/ P6 w+ r4 xBefore concluding, let me venture some additional advice based on my experience:0 b$ q2 Q9 i1 k8 I9 \

# [' N% y0 f B/ ~6 K7 |# [* C= Install the spectrometer in the best shielded room$ R! ?% X8 a D, t. q, p$ L6 J$ [ you can get; the best choice is once again in the basement, where you + g! m8 b: L. ?' yhave the whole building above the ceiling and its [grounded]/ X2 b; K' U7 X2 m8 E) B1 ^ foundations all around the rest, done in iron-reinforced concrete,& S3 G6 ^/ g8 J! F! Q: ]+ {( ?' ^' i: d9 S amounting to a good Faraday's cage at no extra cost.5 _2 y6 r$ X* J h H# ^% ]

5 h& z8 p( |1 ?! U, {, B8 m! k/ c" f = If possible, avoid top floors. If you can't avoid ! c4 S& N- Y6 B$ d. B/ ?going upstairs, take a good look out of the window: if you see nearby0 `. y% a q7 G transmission antennas, get ready for troubles proportional to their . s# U5 v, }' a: R" D1 R gdimensions and closeness (to my knowledge, however, mobile telephony 8 Y) D! @( P# G) ~: fantennas cause so far no harm).7 _ L1 ?, }0 G! p9 |9 N

* v4 g% E( r; D. M+ ^ b% I= I'm sure that an exchange of experiences and/or: T# _4 a6 M8 M! m' r suggestions regarding this matter would help a lot to solve many e: ^8 i+ F$ X( I 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. 3 g8 r r' a$ Q

; V4 I l, z- z4 o9 j Vanni Piccinotti, Firenze, 11 April 2008


摘自stan' NMR Blog.

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发表于 2008-7-2 09:22:51 | 显示全部楼层
see see!
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