Fermi lab

MAGNETIC AND ELECTRICAL PROPERTIES OF ENERGY SAVER SPOOL PIECES

M. Johnson, A. Mcinturff, and R. Raja

November 1981

TM 1076 1620.000

Introduction

The following is a compendium of the magnetic and electrical properities of the first 46 correction coil packages (also known as spool pieces) of the Fermilab Energy saver. Due to the large amount of information available, the emphasis will be to provide a global overview of the plots rather than to examine each property in detail. The magnetic properties measured fall into 5 categories:- transfer constants, harmonics, magnetic centers, coil angles and polarities. Of the electrical data available, we will present histograms of DC resistances of coils, number of quenches per coil and high potential breakdown voltages. The polarities of each coil are checked by the measuring system and if incorrect, are corrected immediately and will not be the subject of further discussion here.

The Cyber Data Base.

The magnetic measurements are performed with the aid of a PDP 11/20 computer. The data is transmitted to the Fermilab Cyber 175 by means of magnetic tape. The electrical data are fed into the Cyber from summary sheets at the prompting of a program( called SUMARYS in the procfil SUMARYS) which checks the data for trivial typing errors and organizes it into a neat format. The magnetic and electrical data are then combined and stored in a random access file called SUMSPUL /UN=94420 which is accessible publicly. The procedure called FORMAT in the procfil SUMARYS /un:94420 allows one to print the summary sheet for any set of spools. Another procedure called SHO in the file SUMARYS runs diagnostics on the spools subjecting them to various rejection criteria as well as enabling the production of histograms of any quantity of interest. The histograms are produced using KIOWA whose output can be graphically manipulated and sent to the Calcomp plotter using the program HISTRRe The plots produced are the result of analysis on 46 spool pieces (see attached list for spool names )

Transfer Constants

Figures 1-5 give the histogram of the transfer constants for the various types of coils used in spool piece construction. The sextupole coil in a DSQ package has different dimensions than that in an OSQ package and therefore they are plotted

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separately. The quadrupole coils are ~dentical in both packages, hence all quadrupoles are plotted in Figure 2.

The spread in the transfer constants in each plot result of two effects. a) the spread in manufacture slight drift in the relative calibration of the two amplifiers used to measure the transfer constants.

is a and b) lockin

One can eliminate the effective of long term drift in the

calibration of the lockin (at the level of 0.5%· or so) by fitting the transfer constants of all the coils in any given

·' spool to a set of standard values by multiplying each by an overall calibration factor. Any residual departure from the standard values woulq clearly be the result of manufacturing errors.

Harmonics

The harmonics measured by the Morgan Coil are with respect to the center of the Morgan Coil probe and are in a co-ordinate system with the x-axis pointing along the horizontal. The harmonic information is used to set the spool piece in the ring with the center of the sextupole on the beam axis. The spools are rotated so that the upstream quadrupole magnetic field is vertical in the horizontal plane passing through the quadrupole center. The harmonics presented here have all been transformed into this co-ordinate system and hence are called ring harmonics. The untransformed harmonics are called Lab harmonics. Figures 6-45 contain plots of various harmonics. The title of each figure is self-explanatory. For instance, Figure 22 is the normal octupole harmonic of the quadrupole coil and hence the title Pole:4, ring harmonics:8, Normal. Since the OSQ and the DSQ sextupoles are similar to each other in angular dimensions, we have not attempted to distinguish them here. Also since we are in the ring co-ordinate system, skew coils will contribute those harmonics to skew plots that normal coils contribute to normal plots. This is particularly evident in plots 44 and 45 which are the normal and skew decupole harmonics of the dipole coil. The dipole coil has a -2% decupole component due to its geometry. Both figures 44 and 45 show a peak at -.02. This is because some of the dipole coils are skew dipoles.

Since we are working in a system where the origin is the magnetic center of the sextupole coil, the quadrupole ring harmonic (normal and skew) of the sextupole coil is

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identically zero by definition. is to be compared with the lab which are broad distributions.

(see figures 27,29). This harmonics (figures 26,28)

A similar effect is evident in the case of coil (Figures 14-17 ) and the octupole coil implying that the sextupole center is closer the quadrupole and octupole centers than center.

the qua~rupole

(Figures 38-41) on average to the Morgan Coil

It must be mentioned that in transforming the harmonics to the ring co-ordinate system, we have assumed that all harmonics above octupole are zero for all coils except the dipole coil for which the ten-pole is also considered.

Angles

Figure 46 is the histogram of the angle of the upstream quadrupole coil when the spool piece is set on the measuring table. Figures 47-52 are the histograms of the angles of the various coils with respect to the quadrupole coil. Figures 47 and 49 thus give the relative angles of the coils in the DSQ package. Figure 50 gives the relative alignment of the DSQ package with respect to the OSQ package. Figures 51 and 52 give- the relative alignment of coils within the OSQ package. Most of the angles are outside tolerances for the early spools. With the use of the electronic alignment technique, the later spools are known to be much better.

Electrical Data

Figure 53 is the histogram of the cold test run numbers of the spools used in the analysis. Figures 54-59 are the DC resistances of the various coils. The large spread in resistance in some of the plots may be due to calibration errors. Figures 60 and 61 are the plots of the number of quenches it took to get these coils up to their operating current. There is some evidence that the OSQ package quench characteristics are a bit better than those of the DSQ package.

There are a large number of hi-pot tests done per magnet and it is not convenient to histogram each high pot voltage. Figure 62 is the histogram of the high pot test voltage between the dipole and sextupole coil of the upstream package in single phase helium at 22psig. The cut-off limit

- 4 -

is at 2.0kv. There are some coils which do not reach this voltage.

Diagnostics

Figures 63 and 64 give the format of the data summarys sheet for a typical spool TSC050. The program SHO analyzes the numbers and if any quantity is outside the tolerance limits (as specified by Helen Edwards' memo) a message is printed. Figure 65 gives the diagnostic output for spool 50.

Each time a quantity falls outside the tolerance, the program generates a fault number. Figures 66-71 are histograms of the various fault numbers. Figure 66 is the histogram of the "TYPE" fault number which indicates whether a spool advertised as a particular type is indeed that magnetically. So far there have been no TYPE faults. Also a spool has yet to fail the criterion for magnetic centers and the harmonics are well behaved. iut the angles and hi-potting more than make up for these instances of good behaviour.

It is a pleasure to thank various members of the Fermilab technical staff, Lou Rolih in particular for carrying out the measurements in question.

- 5 -

LIST OF SPOOLS IN THIS ANALYSIS

SPOOL . TSB013 . SPOOL . TSC014 . SPOOL . TSC016 . SPOOL : TSB017 SPOOL . TSC018 . SPOOL . TSD019 . SPOOL . TSC020 . SPOOL . TSD021 . SPOOL : TSA022 SPOOL . TSD023 . SPOOL . TSC024 . SPOOL . TSD025 . SPOOL . TSB029 . SPOOL . TSD031 . SPOOL . TSC032 . SPOOL . TSB033 . SPOOL . TSC034 . SPOOL . TSC037 . SPOOL . TSF038 . SPOOL . TSE039 . SPOOL . TSB040 . SPOOL . TSC041 . SPOOL . TSE043 . SPOOL TSB044 SPOOL . TSC045 . SPOOL . TSD046 . SPOOL : TSD047 SPOOL . TSA048 . SPOOL . TSC050 . SPOOL TSD051 SPOOL TSE052 SPOOL . TSE055 . SPOOL . TSB056 . SPOOL . TSC057 . SPOOL . TSC059 . SPOOL . TSB060 . SPOOL . TSC065 . SPOOL . TSD066 . SPOOL TSC070 SPOOL TSC073 SPOOL TSD074 SPOOL . TSA078 . SPOOL . TSF079 . SPOOL TSC080 SPOOL . TSD082 . SPOOL TSB083

FIGURE CAPTIONS

FIGURE 1. TRANSFER CONSTANT 2 POLE. FIGURE 2. TRANSFER CONSTANT 4 POLE. FIGURE 3. TRANSFER CONSTANT 6 POLE OSQ. FIGURE 4. TRANSFER CONSTANT 8 POLE. FIGURE 5. TRANSFER CONSTANT 6 POLE OSQ. FIGURE 6. POLE=2 RING HARMONIC=2 NORMAL FIGURE 7. POLE=2 RING HARMONIC=2 SKEW FIGURE 8. POLE=2 ~ING HARMONIC=4 NORMAL FIGURE 9. POLE=2 RING HARMONIC=4 SKEW FIGURE 10. POLE=2 RING HARMONIC=6 NORMAL FIGURE 11. POLE=2 RING HARMONIC=6 SKEW FIGURE 12. POLE=2 RING HARMONIC=8 NORMAL FIGURE 13. POLE=2 RING HARMONIC=8 SKEW FIGURE 14. POLE=4 LAB HARMONIC=2 NORMAL FIGURE 15. POLE=4 RING BARMONIC=2 NORMAL FIGURE 16. POLE=4 LAB HARMONIC=2 SKEW FIGURE 17. POLE=4 RING HARMONIC=2 SKEW FIGURE 18. POLE=4 RING HARMONIC=4 NORMAL FIGURE 19. POLE=4 RING HARMONIC=4 SKEW FIGURE 20. POLE=4 RING HARMONIC=6 NORMAL FIGURE 21. POLE=4 RING HARMONIC=6 SKEW FIGURE 22. POLE=4 RING HARMONIC=S NORMAL FIGURE 23. POLE=4 RING HARMONIC=B SKEW FIGURE 24. POLE=6 RING HARMONIC=2 NORMAL FIGURE 25. POLE=6 RING HARMONIC=2 SKEW FIGUR.2 26. POLE=6 LAB HARMONIC=4 NORMAL FIGURE 27. POLE=6 RING HARMONIC=4 NORMAL FIGURE 28. POLE=6 LAB HARMONIC=4 SKEW FIGURE 29. POLE=6 RING HARMONIC=4 SKEW FIGURE 30. POLE=6 RING HARMONIC=6 NORMAL FIGURE 31. POLE=6 RING HARMONIC=6 SKEW FIGURE 32. POLE=6 RING BARMONIC=B NORMAL FIGURE 33. POLE=6 RING HARMONIC=8 SKEW FIGURE 34. POLE=S RING HARMONIC=2 NORMAL FIGURE 35. POLE=S RING HARMONIC=2 SKEW FIGURE 36. POLE=S RING HARMONIC=4 NORMAL FIGURE 37. POLE=S RING HARMONIC=4 SKEW FIGURE 38. POLE=S LAB HARMONIC=6 NORMAL FIGURE 39. POLE=S RING HARMONIC=6 NORMAL FIGURE 40. POLE=B LAB HARMONIC=6 SKEW FIGURE 41. POLE=8 RING HARMONIC=6 S~EW FIGURE 42. POLE=8 RING HARMONIC=B NORMAL FIGURE 43. POLE=B RING HARMONIC=8 SKEW FIGURE 44. POLE=2 RING HARMONIC=lO NORMAL FIGURE 45. POLE=2 RING HARMONIC=lO SKEW FIGURE 46. U/S QUAD ANGLE DEGREES IN LAB. FIGURE 47. U/S POLE=2 ANGLE DEGREES IN RING. FIGURE 48. U/S POLE=4 ANGLE DEGREES IN RING. FIGURE 49. U/S POLE=6 ANGLE DEGREES IN RING. FIGURE 50. n/r::. "D0LE=4 ANGLE DEGREES IN RING. FIGURE 51. D/S POLE=6 ANGLE DEGREES IN RING. FIGURE 52. D/S POLE=S ANGLE DEGREES IN RING. FIGURE 53. SPTF RUN NUMBER FIGURE 54. AB-DS SEXT OHMS FIGURE 55. DE-DS QUAD OHMS FIGURE 56. GH-US QUAD OHMS FIGURE 57. KL-US SEXT OHMS FIGURE 58. NP-DS OCT OHMS FIGURE 59. RS-US DIPL OHMS FIGURE 60. NUMBER OF QUENCHES DSQ FIGURE 61. NUMBER OF QUENCHES OSQ FIGURE 62. UPSTRM COIL HIPOT D/S FIGURE 63. MAGNETIC DATA SUMMARY FOR SPOOL-50. FIGURE 64 (A), (B) ELECTRICAL DATA SUMMARY FOR SPOOL 50 FIGURE 65. DIAGNOSTIC OUTPUT FOR SPOOL 50 FIGURE 66. MAGNET TYPE FAULT NUMBER. FIGURE 67. MAGNET ANGLES FAULT NUMBER. FIGURE 68. MAGNET CENTER FAULT NUMBER. FIGURE 69. MAGNET HARMONIC FAULT NUMBER. FIGURE 70. MAGNET HIGH VOLTAGE FAULT NUMBER. FTr.TTRF. 71 - Mn<:NF.'f' 't'O'f'n r. Fnnr.'t' NT1M'RRl1

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S/G!l S/GO SI~ -----------------·------~---------~---o/Gfr··· - OIGft-···------- SM · ·-·-·---------------·--··

POST TEST tN HJTROGfll AT AHAIENCE.

------···-··-··--·--···----

•••••• fllAGlll'T SUfll'4lllY •+••• 505111

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TE'!PEllATUllECKI 40 6 TE'!Pf.RATUREl~I 4.6

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··································································~~······························································· DTIGNOSTICS FOP SPOOL• rsno,7 N4GN~T JS TNOFEO TYP! D

•••••••••••••••••••• ANr.LE ANU CFNTER CRITERIA AP~LJED PnLE • UPSlPFAM/OOWNSTPEAM MO'.!lftJM Pl''IMJSSTql"'. ANGLE = POL" t, llPSTPFAM/OOWNSTRFAM MAXTMUlf P!~N!S~!~LE ANGLE :

? 11AS ANGLE = .'570110 OEGRF.ES

-z HA<; umlf: = 1.1sooo ne:r.REES

1.06887 DEGREES

~~~~~ le 30723 OEGREES

-~•••• .. ••••••••••••• HAPMCNIC ~RITEPTA APPLTEO -----------·--···-- -~-·- -

•••••••••••••••••••• 111r.11 vrLTIGE CRITERIA APPLTEO -··· - -··· ~ -- .

.... "'!r:tJLO l l n1nn HEL TUM 7!~USS LEAD~ +/GO ?..60 IS LOWER THAN THE LIMIT 3.00 ••• ~CrLO ~TOUT'l Hft!UN ?.UPSTREAM COIL S/GD 1.30 IS LOWER THAN THE Lil'ltT ?.oo ••• ~f':Ol'l !011!'1 HFL tUH Y.COWNSTREAH COIL 0111 1.~o IS LOWER THAN THE LIH!T ::-.oo ---· ?.f':rLn lT'lU!'I Hfl'U"' 1'"0HN<;TREAl1 COIL-- -·- - Q/GO ------ -- ----- t.70 IS LOW~R THAN TME LIMIT ?. Oil •n itr:nln L tnut'l HfLtUH "'!UPSTREAHICOHNSTREAH SIO t.~O IS LOWER THAN THE LIMIT ?oOO ••• tCrLO lTOU!O HFLtUH YUP~TREAH/OOWNSTRFAM SIS t.JO IS LOWER THAN TH! LIMIT ?.oo ••• 'l!COLD lt!lUT'I HELIUM "f.UPSTREAH/OOWN<;TREAM Siil t.~O IS LOWER THAN THE LIMIT ::-.oo

; ......................................................................... *•························································· nrar.NllSTtr:c; F'IQ SPOOL• TSA0•8 MAt.N~T TS T~O~En TYPE A

•••••••••••••••••••• ANr.LE ANO CENTER CRITERIA APPLIED

•••••••••••••••••••• HARMONIC CRITERIA APPLIED

••••••••••••••••••••HIGH VOLTAr.E CRITERIA lPPL!EO

-•••-·'P.~H!'"<?T - 1 PHASE tffLIUH AT AHl!!ENCEo ••• 'l!PRETFST - t PHASE HFLlU'4 AT AHfll!'"NCE.

'!PUSS LEA~S------- +!--------·--------·----· e 70 IS LOWER THAN THE LIMIT · - - t.~o ·-----~-Y.llUSS L!'"AOS +/GO .70 IS LOWER THAN THE LlHIT 1050

••• Y,PRETE~T • t P11AS! HELIUM AT AH•TENCE • ••• "l!Cntn L Tflll!O HFL ttJM

7!flllSS Lt::AOS •/GO .70 IS LOWER THAN THE LIMTT 1.so YPUSS LEAns +/• t.oo IS LOWe~ THAN THE L!H!T J.oo 7!1!llSS LEADS -- -- +/Go ·-- 1.10 IS Lowe~ THAN TH!' LIH!T :<.oa ••• "'!C~l'l LTl)l~O HELIUM

._,. V.~rtri l !fltf!ll HFlit1'4 ••• ')!O~ST Tf<;T !N N!Tqnr.EN AT ~MRTENCfo .... ~PO<>T TF"<;T TN NTTonr.fN AT IMR!~NCE. ••• "r.PO<;T TEST TN NtToor.FN AT aHq!€HCE.

TNVALtn OAT6 n-r.Pn:TNF! L!NF" NUHnF~ TNVAL!O OAT• E-r.oo=INFI LINE NUMRER

?.PUSS LEAns •/GO 1o10 IS LOWE~ THAN TH! L!H!T ?.PUSS Lf'Ar.S +I• 1 0 RO IS LOWCR THAN TH~ Ll~tT ?.!!US<; LE ACS +1r.D ?o10 IS LOWoF! lHAN THE LIHIT 7!PUSS LEAM -------- •/GO ·------------ - -· ?..l+O IS LOWC'R THAN THE LIMIT

~o sPontt ncoi;o H SPOOlt TSCQSO

"l. 0 0 ?.OO 3.10 '.'!.DC

··················································~···••••¥••••································~··································· ntar.NOSTtC<; FOO SPOOL• TSCO~~ MAr.H!'T ye; !NO!'EO T¥PF C

•••••••••••••••••••• ANr.LE ANn CENTER CRtTERtA APPLIED PnL f l+ ll"Sl'DE AM l'lOWNSTF!F.:A H HAY!WUH PFoH!<;STRLF ANGLE = POLI'' "- llP<>T11FAM/'IOWN<;TPEAM MAXIMUM PEPMJS~YBLF ANGLE :

? 11AS ANGLF.: : .t;7000 l'lF.GoE"'S

? HAS ANr.L E = lo \t;O 00 UEGREES

•••••••••••••••••••• HARMONIC CRITERIA AP~liEO

~ o I! 26 01 OEGRE€!;

-t.38778 OEGPEES

_..• .. ••••••••••••••• Htr.H VOt..TAGE CRITER1A APPLTEO ----~ - ·-·· - -· ·-·--

••• Y.MLO L TflHTI' Hfl!Ull ?.UPSTREAM COIL S/GD ••• '1.COLn L!OIJ"O HFlJIJI! '1.rOWNSTREAH COIL O/S

-- ••• 't.f':CL ri L rn1rrn 11E tUll 't.COWNSTREAH COIL OIGO -- ···~ . --••• '1.Cntn LTOll!fl HFL!UH "'!OOWNSTREAH COIL O/GO H• "'!C'll(I L !l'llTO Hfl!UH 't.UP~tR~AH/COWNSTREAH SIO •n "'!COL'l L TOUTO HEL !HM "P.UPSTR~AMlnOWNSTREAM SIS

- ••• 7!00LO L Ifltll!l· HfLIU!1 '1.UPSTREAH/r.OWNSTREAH OIS --·-·----·

1.70 IS LOWER THAN THE LIMIT 2. 00 t.qo IS LOWER THAN TttE LIH!T "· 00 - 1.qo I~ LOWiOR THAN THE L !H!T ?oOO t.AO IS LOWER THAN THE LtH!T ?. 00 t.40 IS LOWER TH~N THE LIMIT "· 00 1.ao IS LOW!R THAN THE Ll"IT ?. 00

+··-- - 1 0 70 IS LOW~R THAN THE LIMIT 2.00

···················································································~·····~···~·················~··4················ nu r.Nnsi'rcs FOP. SPOOL' TS0051 -~AGNtT !~ ~NOrE'l TYP~ 0

•••••••••••••••••••• ANOLE ANn CENTER CRITERIA APPLIED

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