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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. ?: r) r! C" q7 ?4 |& q: y This applies to all kinds of spaces, including the electromagnetic( I6 U7 y' O9 c& c3 f, C ether. What follows is a contribution and a warning from Vanni Piccinotti,- O: n& o" z6 T* m an engineer based in Florence, Italy, who has decades of experience & [; S% b0 n8 y6 J# Owith installing, testing, and servicing NMR and EPR spectrometers. The # T. M+ L& b) [6 N% O3 Y; Vproblem of RF interference has never been trivial and it keeps slowly4 b: h- b9 r7 B1 m! Z but inexorably mounting. The spread of urban areas (combined with the: A& c1 Q# O" a tendency to install MR instruments in those same areas) and the2 T0 ~4 ? Z' ~ mounting maze of wireless technologies penetrating our daily life spell 6 l! _' ^7 G" N+ u( t) y$ Cnothing good for the future quality of our NMR signals. With concurrent ( m. D# O: m6 G& Q Cprogress in basic sensitivity of the instruments, time might come when - @ i3 w- V/ Q9 z+ k$ @1 f0 C% ?environmental RF noise will be the single major obstacle to further7 s2 }' `! A- s6 ~- W4 W3 w5 c progress. 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
 

+ v$ w0 ?7 o' U* Q7 z( m" tCross-talk between FM Broadcast Radio Transmitters (88-108 MHz) ; f2 f; F2 ?0 H7 i+ A# Zand NMR Spectroscopy: A recent experience ' P& x- c8 u$ I4 y

- K" ^# [6 s1 t- n Recently I had to install a 400 MHz (9.4 T) NMR Spectrometer. The 7 O5 `8 d* u% F- T/ N) j0 qsystem worked fine and, using an Indirect Detection Probe , met quickly( E/ t* D+ T) |% m% L& m4 M2 b and effortlessly the specifications. But later on, when the customer$ O# m+ x h' D9 @7 b& ~# { installed a 13C direct detection Probe, the S/N ratio turned out to be . q9 M. H; t9 J" d/ b/ p5 M- m ~1 lquite low and, on top of it, the sensitivity was subject to erratic and ! v0 |: F8 A& m! H* G4 ?2 z" G8 Wvery large variations from 50:1 to 130:1 (manufacturer's specs give9 c% F: O% U& S3 g8 N$ n 155:1), without any apparent reason.* z! X; @' D j8 }2 v) h8 x' Y8 u. E

Since the nominal 13C observe frequency at 9.4 T is 100,5682 Z+ g+ _6 r/ `0 _5 X4 c MHz, right in the middle of the range of commercial FM broadcasts, I 0 ^% P' r& e$ Y. F; xhave immediately suspected that the spectrometer was picking up one of 7 Y# o" X1 l! e% r8 Ithose radio stations. In fact, using a cheap FM radio receiver, a 9 \( n; W/ ]) Y* | l n. Astrong station was quickly found at 100,60 MHz. At this point, I have( R3 a3 Y3 ]8 T) H% g7 ^ connected a simple audio amplifier ending with a loudspeaker to the 4 V& @ V2 H ]2 e3 \0 {output BNC of the observe receiver which was there apparently just for; c) U. `0 _$ j this purpose, and all of us were listening to the radio using a 200.000 $ ?; Q1 E5 y ]( E) iEuro NMR spectrometer, except that the audio quality was really poor, + H) a, y* g$ M7 j0 gmuch worse than from the above-mentioned gadget radio (a shopping mall% ^0 {6 e( G* r% {: c2 K gift).: w [2 S" }" r$ {

The problem is well known from the old times, when the highest : `4 ]$ t7 _; ufield was 2.45 T and the nominal H1 frequency was close to 100 MHz. One + W/ H- Q- }$ S1 Dof the first Italian NMR spectroscopists to experience it, back in 0 @+ D% `/ @2 _) ]1974, was Prof. L.Lunazzi at University of Bologna, on his brand new M2 e1 ~, ]* j8 @, _Varian XL100 spectrometer, and the radio station was Radio San Luchino, : r1 p( H1 L8 F o5 R6 r; h8 o7 Iwell known to anybody living in Bologna, which broadcasts from the top1 m" i0 b# ? q; K of the nearby Saint Luca hill. 3 ]/ ~) R6 J' P% Q% g& {: l

The obvious solution is to change the magnetic field, and thus : X; W% ~3 u6 |5 Rall resonance frequencies, in order to get out of the modulation / `: m/ M" K! c) F2 ^5 k( s; Genvelope of the interfering transmitter. But this is not always easy,) n- V5 D# x) h$ X2 Y: `. q since the range by which one can move the magnetic field changing just ' G' b4 N0 ?2 \& r, d$ rsome software parameters is usually limited to a few tens of kHz in the / w. `: C( z9 y8 u- r) ~frequency domain. If larger variations are required the poor engineer O- ` l* n% a h9 shas to work on the superconducting coils of the magnet, which is a 6 Z n( k, N# n+ ^% {no-trivial job entailing the risk of a total or partial quench. 0 C, U6 W* `9 G% C( u A

Bitter experience shows that persuading the involved radio6 i) e( A+ n$ |" {0 p; T station to change its operating frequency is a time consuming,4 m O- Y3 x3 g+ t frustrating, and apparently quite impossible task.0 {0 D% l v6 o8 p5 U9 W& A( _1 Y

Being well aware of the problem, my preliminary spectrometer$ h# D7 r/ R$ U! e1 t: A checks always include some blank acquisitions taken before running up. |7 }- |. u/ D) `( O; G9 g the magnet so that there is no chance to observe an NMR signal. The8 w a0 c1 b3 ^1 ~ Q resulting dataset should be pure white noise, without significant% n" H; m6 @3 V( F spikes. This was done also in this particular installation but, as 3 N& h, u5 w- Y+ @usual, in the days following the energization the magnet drifted a bit,9 h5 d3 |# b2 s( Z" D; ~7 s getting closer to the radio station carrier. Furthermore, the usual 13C 2 p1 h$ ]$ h) m) ~spectral widths are quite wide which makes things even worse. Murphy's , k. v' o& S5 s; sLaw has no exceptions! 3 ?) m! Z& J6 B; x7 X! L G3 K

But we are just at the beginning of my real troubles. Before 2 P4 R0 ^2 d; i" j! y1 O# hputting one's hands on the magnet, one should better know how much, in$ D+ {6 t4 \/ _4 n9 i! h. ~* z which direction, should the field be moved. I have therefore used a$ J$ ?6 r8 {0 z# P9 d/ X7 ] good Spectrum Analyzer (Tektronix model 2710) to check the frequency1 j# Y: z. q5 o+ \( O( G! c spectrum around 100 MHz, ready for the worst. And the worst was what I , @0 h9 w0 e' qgot! The band was filled with FM signals, evenly spaced by 250 kHz and + I& g4 Q& _* K D' Iwith modulation envelopes as wide as 100 kHz, so that when I got far : a! S7 D1 U. A% kfrom one station I started receiving the next one; accounting for- L+ w' a8 [/ V3 P$ R3 r folding and aliasing effects, there was no chance! The only somewhat5 y; _' r3 F( d ^6 P' c* y free region was at 100,120 MHz, but this implied proton frequency of 4 [/ G, k% L0 t6 Z$ j398.100 MHz. So now the spectrometer is no longer a "400"!: ~" @7 e% e4 o1 i

Before installing a spectrometer, you better get a Spectrum/ V) N! S: o! a |7 [ Analyzer and check for the presence of RF fields in the instrument + t" W r3 K9 W. d0 eroom, taking care to explore the areas close to the observe frequencies" v, E! n7 \4 }' j of all the most important nuclei. Don't forget the lock: at 14 T ' Y4 q8 p! L$ L: G& g, c6 f(nominal 1H frequency of 600 MHz) 2H resonates at 92,095 MHz, once3 h" h& H* e& W4 D again in the FM broadcast band. The lock channel receiver has quite 8 D. B. A. ^8 R- _2 C z2 f* Qnarrow bandpass filters, so hitting a radio is a really bad luck, but6 k2 T5 O( ~8 G7 \0 ~ it had already happened, resulting in fast lock level variations and( D3 f* \) }% r& A, t- g6 q* D# t totally malfunctioning Gradient Shimming which uses deuterium as- @: s! a0 E% Z7 L" P0 N observe nucleus! ~: y( [! Z1 @6 e1 S

Needles to say, the extremely high sensitivity of an NMR B4 Y' B' }/ s% n# C1 aSpectrometer shows up. The signal from the guilty radio, as observed on R) Y3 u( f, ^# K/ I4 _5 q the spectrum analyzer inside the spectrometer room, had very low9 f2 Z3 H& l# h' y0 E intensity level of about -70 dBm, some microvolt/meter, but that was / k; v1 P0 x N3 \; }4 x: henough to almost completely hide the quite strong 13C signal from the8 f/ Y1 m" c2 F# U ASTM sample!2 Y6 D( }/ V9 d+ @6 Y$ J0 ]- M, e

The radio was clearly picked up by the Probe (closing the9 n/ I7 z) Z6 G4 x4 X* v Preamplifier input with a shielded 50 ohm RF load, all signals 6 }+ F7 _9 g; mdisappear) but, quite surprisingly, there is almost no shielding effect 7 k7 K' Z( ]3 iattributable to the metal body of the magnet, which is after all an 6 l k: p7 o! t" nalmost completely closed cylinder all around the Probe. Most probably a 0 T7 k+ T& \& Y: K5 \good deal of the signal leaks in through the Shim Coils which are; A, E* x2 W- A0 ~3 |( j mounted very close to the Probe and, together with their connection % {. P7 J" C R/ ocables to the Console, constitute a quite good antenna. * B! b7 W8 @4 k0 d/ f

Too bad the Shim Coils are essential, and effective shielding 9 S' `, O8 {1 |/ q% G4 bof the instrument with a Faraday's cage is always difficult and : m( s8 O/ s) I9 Lexpensive (it may be almost impossible once the spectrometer is 9 o, Z% H. }- f' B$ Einstalled).' l, ]+ G; X+ }7 [7 h! R5 ~) e" y

" ?4 c( I O" h; L$ l Before concluding, let me venture some additional advice based on my experience:' L1 _5 ~7 |$ C! D' S2 n5 i

8 v& q% g$ p' @2 e8 f" i= Install the spectrometer in the best shielded room 8 P W$ ~. t$ S/ z# ayou can get; the best choice is once again in the basement, where you0 y! S* }8 i. j# d3 y have the whole building above the ceiling and its [grounded] + v. J9 v1 R% U& y* `1 q- Xfoundations all around the rest, done in iron-reinforced concrete,7 O+ W% b1 V, r# b3 V1 y/ r" ` amounting to a good Faraday's cage at no extra cost. ) L4 H# U* J" z& }, g

P2 a- [ w9 E6 p4 Q. \! l& _8 U = If possible, avoid top floors. If you can't avoid# V. \" K Y+ B going upstairs, take a good look out of the window: if you see nearby, O% p$ H0 A, K% y" z transmission antennas, get ready for troubles proportional to their- d9 ~* y4 s1 b0 P$ _( `( M dimensions and closeness (to my knowledge, however, mobile telephony6 @; H7 M+ N: D! P antennas cause so far no harm). , S/ ^. R8 T: c

% T4 w6 V% h6 Y& t M# n= I'm sure that an exchange of experiences and/or + X7 Z, o8 \% e6 d* Asuggestions regarding this matter would help a lot to solve many W5 B% o, i# ]* v- X0 Jexisting 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. : @& C4 d9 z( M8 Z3 y% ^( B

2 j" W/ ^7 V n5 j, B- e% q 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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