ts-ssc 90-002 fnal::jbs 28-mar-1990 22:31:00.77...
TRANSCRIPT
From: To: CC: Subj:
FNAL::JBS 28-MAR-1990 22:31:00.77 BOSSERT,CARSON,HANFT,Wt<OSKA,MANTSCH,MAZUR,PEWITT MYSELF 050307 and oso~oa preloads explained?
TS-SSC 90-002
From the measured coil sizes, collar size and amount of Kapton added to the standard ground wrap the expected prelodd for 050308 is 8 kpsi in the inner coil arid 11 kpsi in the outer coil. The actual prestresses are about 2 and 3 kpsi respectively. This may result from either the coil being smaller than we think it is or the collar cavity being larger than we think it is. The former would result from some as yet not understood systematic error in the coil size measurement. The latter might result from a mis-design or mis-measurement of the collars, poor tolerance on the thickness of the ground insulation or the Kapton ground insulation flowing into the die-break of the collars.
These would have different effects on the harmonics . If the coil is too small but the collar cavity is correct, the coil will require less than the expected prestress but will end up at or near the design location. If, on the other hand, the cavity is too large, the coil will occupy a larger azimuthal space than called for in the magnetic design and therefore the harmonics will be altered.
The measured body field sextupole moment of 050308 (measurements taken today by Hanft, Koska, et al using the mole) is -6 units. Gerry Morgan calculates that increasing the inner (outer) coil collaring shim by 1 mil increases the sextupole moment by 0.49 (0.41) units. That is, if both the inner and outer coil cavities are 1 mil smaller than the design value, b2 wil I be +0.9 units. To generate -6 units would require the inner and outer cavities to be 7 mils too large (assuming an equal error in both).
I put such a collar size error into the spread sheet that is supposed to calculate prestresses from coil sizes. Lo and behold, the predicted prestresses are 2 and 3 kpsi on the inner and outer coils. On the final collaring of 050307 the measured prestresses are about 5 and 7 kpsi in the inner and outer coils while the predicted prestresses are 11 and 13 kpsi. If I increase the collar cavity by the same 7 mils, the predicted prestresses drop to Sand 5 kpsi.
The closeness of the agreement between calculation and measurement is probably somewhat fortuitous given all the fine points that I have ignored in this argument. Nonetheless, it suggests that the coil size measurements are more or less correct and that the collar cavity is to blame for the low preload. Stuffing more Kapton at the poles of 050309 will probably not only increase the preload but also set the harmonics to the correct value. It had been my intention to set the amount of additional Kapton by seeing how much I would have to alter the collars on 050307 and 0$0308 to get the observed preloads. The mole measurement seems to have given me a good way to get the correct value on the first try.
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<1-14> •i1 n ...
lOOOOOOO( -0.0008 -0.0008 -0.002'
lOOOOOOOC -O.OOll7 -0 .0017 -0.0011
lOOOOOOO( -0.0011 -0.0040 -0.0025
lOOOOOCXX -0.00ll -0.0021 -0.0040
lOOOOOOO(
-0.00M -0.ooto -0.0024
lOOOOOOO(
-0.00IO -O.OOl1 -0.0011
lOOOOOOO( -O.OOll7
-0.0017 0 .0007 0 .0011
-O.OOll7 0.0009 0 .0022
-0.0022 0.0009 o.oou
"1. -0.00D 0.0010 o.oou
lOOOOOOO( IO.IO ID.ID 21.71
lOOOOOOOC 25.11 28.11 :11.40
lOOOCOOCX 27.tl 22 .19 M.•
)0000000(
14 .• 25.54 22.19
lOOOOOOO(
D .14 17.44 ....
lOOOOOOO(
25.07 14 •• 17.'1111!
lOOOOOOO( 15.11 .....
'""' 10.1
••• lOOOOOOO(
11.1 11.0 11.0
lOOOOOOCX 12.1 11.1 10.2
lOOOOOOCX 9.4
10.9 11.4
lOOOOOOO(
11.4 6.2 9.2
lOOOOOOCX 7.1 9.1 I . !
lOOOOOOO( 1.4 9.7 ••• lOOOOOOCX 7.7 7.5
10.1 lOOOCOOCX
9.1
t .114414
C.ilf Slii•:
a\r•• aiu
10I llttf DSOIOI 1/4 loc 1-r o.ooa c.11 .... ,.,, o IOOO IOOO 10000 12COO
O.OOl2 0 .0071 0.0061 0.0047
lioror f i\ o\f•• • f(ein) o(O) • 19.'8 k,.i •/d1 • -1.71l6 kpei/•il
oolfortd ot•-7 .7
C.ilf Slli• :
s\r"• eiz1
107 llttf DS0101 1/4 loc h•tr o.ooa Col lor .,,.,, o 6000 IOOO 10000 12000
o.OOft O.OOl9 0.0067 0.0045
lioHr fi\ otruo • f(oize) •fOl • 19.54 k,. i •Ju • -1.NI k"9i/ai I
oal ored o\rt• 7.1
Co I If '°' ""' DSOIOI 1/4 IK °""'' 51.h: 0.010 Collor error: -0.001& otre• IOOO IOOO 10000 12000
ein o.~ 0.0087 o.oon 0.0010
lioHr fi\ otrt• • f(oia1) •fO) • 29.0I hoi .f./d.. • -2.4'4 k"9if•i I
.. , trtd """" 11.1
C.ilf Sloi•:
1\rt• 1iz•
IO& llttf DSOaOI 1/4 loc on.r 0.010 Collor error: -0.0015
IOOO 8000 10000 12COO O.OOM O.OOl1 0.0074 O.OOll
liour fi\ .tr- • f(oin} e(O) • !7.24 k,.i .f./rls • -2.171 i,.i/ail
.. 1 r1r14 a\re• 10.2
Collor oo•li•oct Ci• h,... of .. ., ... i-......wr •il Wt•) Collor .. rt.la I oflot\ (iodi•i••I oollor ~ f,_ -•\ c1owr) d./• a 0.116 •i la/kpei s(O) • 2 •ii•
Coi I ""'• otr•• • f(oollor def11c\i•) o(O) • -1.&7 kpei d./d1 • 1.781 .,.i/ail
A"ntt of 4 ooilo: o(O) • 21 .91 kpei
C.llor nrt.icol rodi .. : 7.2 ai lo
Aver ... inner otrt• • 7.1 Anntt outer otrt• • 10.9
Awtntt ooil otrt•• 9.1
Coilf Shi•:
.t.r•izt
10& llollf DSOaOI 1/4 loo l•n•r o.ooa Collar error: -0.007 6000 8000 10000 12000
0.0012 0.0001 -0.0012 -0 .002J
lionr fit st.re .. • f(oizo) 1(0) • 8.0li kpei O./d• • -1.706 kpei/ai I
oollarocl .t.ro• 2.2
Coi If Shi•:
.tr•• •b•
107 Mogf DSO.tOI 1/4 loo lnnor o.ooa Collar orror: -0.007 6000 1000 10000 12000
0.0012 -0.0001 -0,0011 -0 .002S
linnr fit .tr••• f(oizo) 1(0) • 7.t7 kpei m/rlx • -1.111 kpei/ail
oo llarocl .t.ro• 2.1
Coilf Slli•:
.tr•• •ize
I04 M1gf DSOaOI 1/4 IK 0..tor 0.010 Col lor orror: -0.0085 6000 9000 10000 12000
0.0024 0.0017 0.0008 0.0000
I innr fit ri.ro• • f(obo} •COl • 12.04 kpei m/u. -2.4'4 kpei/•il
oeH•nd •tre• I.I
Coilf Shi•:
st.re• •iz1
I06 M111f DSOa08 1/4 loc Out.or 0.010 Col lor orror: -0.0085 6000 8000 10000 12000
0.0019 0.0011 0.0004 -0.0007
I innr fit .t.ro• • f(1in) 1(0} • 10.&0 kpei m/dx • -2.111 kpei/•i I
oo!farocl .t.ro• 2.4
Dato 1/IJ'IO
Doto 1/8/'IO
Dito 1/2'#'!0
Daw 1/21/'IO
Collar CIO.,li1nc• (in \tr'• of IYI ..... inntr+"Ofilt.er ooil ftr ... ) Coll1r vort.ie1I offoot (individu1I oollor •••1 fro. -•t oontor} clx/• • 0.56 ai 11/kpei a(O} • 2 ai 11
Coi I •••...- .t.ru1 • f(ooll1r dofloc\iOft) 1(0) • -a.57 kpei •lclx • 1.7815 lipei/1i I
"'''- of 4 ooi la; 1(0) • 9.114 .,..;
Coll1r vort.i .. r ••• u .. : ••• 1il1
Avtr ... inner s\r•• • 2.1 Avon.go out.or ot.roN • 1.0
,1.,,.._ .,.; I .t.ro• • 2.1
J5
C.i If 104 llotf DSOI07A 1/4 IN U Do\o 1/IQjWJ ,.. t - 8000 - - 8000 - - 10000 - - 12000 -
•ii .nor •ii onttr .,. i( .nor •ii •8\or 1 )0000!~ O.OllO 0.0152 t ., 0.0267 O.Olta 0.0241 O.OllO 0.0218 0.0187 0.0194 0.0152 2 • 0.0242 0.01115 0.022& 0.0175 0.020& 0.0114 0.0194 0.0152 I )OOOOOt~ 0.0191 0.0152 4 ~OIOO( O.o:tOI 0 ,0152 ' ., o.cm. o.0111a o.om 0.0190 0.0212 o.ou1 o.0205 0.0152 I • 0.02J4 0.0116 0.02JS 0.0175 0.0220 0.0114 0.0206 0.0152 I lOOOOOOOOOOOOOO'OGOOOOOOOOOI)") m IOO< 0 .0194 0.0152 7 )OOl))OOCIXWX~ 0.0190 0.0152 • "' 0.0261 0.01'11 0.02!4 0.0180 0.0215 0.0157 0.0191 0.0152 • .. 0.02 .. 0.0185 0.0220 0.0175 0.0204 0.0114 0 .0191 0 .0152 • ~ 0.0186 0.0152
10 ~ 0.0200 0 .0152 11 ., 0.0277 0.01.. 0.02$7 O,OllO 0.0227 0.0167 0 ,020I 0.0152 11 ., o.0250 o.01es o.m1 o.om 0.0215 0.0114 o.0201 0 .0152 12 ~ 0.0201 0.0152 11 ~ 0.0201 0.0152 14 op 0.0261 0.01 .. 0.0217 0.01IO 0.0214 0.0117 0 .01• 0 ,0152 14 • 0.02N 0.0185 0.0217 0.0175 0.0200 0.0114 0.01• 0 .01'2 15 ~ 0.0111 0.0152 11 ~ 0.01• 0.0152 11 ., o.0262 0.01.. o.oua o.01ao 0.0210 0.0157 0.01• 0.0152 17 .. 0.02$4 0.0116 0.0215 0.0175 0.0199 0.0164 0.0186 0.0152 11 ~ 0.01'1 O.OIU 19 lllOOOOOOOCOCOCQJOOCOOOOOCOOOO«XXX 0.0191 0.0152 20 ., 0.0271 0 .01ta 0.0242 0.0180 0.0211 0 .0167 0.0197 0.0152 to .. 0.0241 0 .0116 0.0221 0.0175 0.0205 0.0114 0.01'7 0.0152 11 ~ 0.0117 0.0152 ZI ~ 0.0186 0.0152 ti •P 0.0261 0.0191 O.OU9 O.OUIO 0 .0215 0.0157 0.0190 0.0152 ti • 0.0241 0.01• 0.0222 0.0175 0.0204 0.0114 0.0190 0 .0152 t4 ~ o.01n 0.0111 '- I 8000 8000 10000 12000 S(lc.G) rY .tr •VII .tr ,._ I
•il-aner •ll-r ... 11-n.r .,.;1-r (oollor) (i-r) 1 t ., o.0074 t .. 0.0057 a 4 5 ., 0,0085
' .. 0.00'9 I 7 .. , 0.0068 1• 0.0054 9
10 u ., 0.0084 11 .. 0.0066 12 11 14., o.oou 14 • 0.0051 1$ 11 17., 0.00'9 11 • 0.0049 11 19 20., O.OOll 20 .. o.oosa :n 12 u., 0.0070 ta• 0.006& 14
IP: ( t-11> 0.0071 •i1 O.OOOI ..... 0.0011
<14-21> 0 .0071 .;, 0,0007 ..... 0 .0015
( 2-21> 0 .0075 •i1 O.OOOI " ... 0.0011
DIMI : < 1-11> 0.0061 •it 0.0007 ..... 0.0015
<14-21> O.OOSI .1, 0.0004 0.0007
< 2-21> 0.0057 •i• 0.0007 ._ 0.0020
o.oou 0.0041
0.0045 0.0080
0.0069 0.0045
0 .0077 0.0056
O.OOl57 0.0042
o.oou 0 .0040
o.ooa 0.0048
0.0069 0.0047
0.00.1 0.0011 O.OOl2
0.0061 0.0004 0.0009
0.0069 0.0009 O.OOl2
0.0062 0.0007 0.0011;
0 ;0044 0.0004 O.OOOI
0 .0048 0 .0007 0.0020
o.ooa 22.54 1.a 1 .4 9.9 1 0.0051 0.004! 25.0I 1 .7 •.I 10.0 2 O.OOl9 lOOOCOCOC ~
0.0044 25.45 1.7 9.7 9.8 • o.oosa 21 .u 1.1 11.1 l0.4 •
0.0065 0.0054 27 .21 • •• 11.1 11.7 5 0 .0056 lOOOCOCOC lOOOOOCOOOOOOOO Ol))l))l)))X
0 .0042 25.08 I.• I.I 10.• I O.OOll 24.81 1.7 8.1 10.S 7
0.0048 O.OOl9 24.54 1.4 9.2 11.2 8 0.0040 JOOOOCO()( lOOOOOIXXlOOOOO
0 ,00&4 21.U 8.2 8.7 10.1 9 0.0041 21.17 1.5 10.7 9.9 10
0.0080 O.OOl51 21.72 8.5 11.1 9.7 11 0.0061 lOOOCOCOC XIOOOOilOOOOOOO
0.0049 :M.11> I.I 11.1 9.7 12 0.0049 21.lli 11.1
0.0047 O.OOll 21.99 I.I O.OOll lOOOCOCOC lOlOOOlOCOOOCiO
0 .0029 22.72 7 .• O.OOIO 22.90 1.0
o.0048 o.ooaa 21.45 1.1 0.00&6 lOOOCOCOC lOOOOOOOCOO)OOO
0.0041 24.'JO 9.1 0 ,0044 25.45 9.2
0.0049 0 .0045 25 .U 9.4 0.0041 lOOOCOCOC ~
o.OOlli 21.11 1.0 o.ooaa a .45 1 .1
0.0048 O.OOll 24.M 8.5 0.0040 lOOOCOCOC ~
0.006& O.OOOI 0.0017
0.0047 o.oooa O.OOOI
0.0051 0.0007 0.0022
0.0047 0.0008 0.0017
O.OOll o.oooa O.OOOI
0.0042 0.0007 0.0021
0.0019 20.90 5 .1
0.0047 0.0007 0.0015
O.OOll 0.0005 0.0012
0.0042 0.0007 0.0021
.111.1. <1-%4> 0.0040 . ;, 0.0009 ,_ o.ooa1
Coilf ,_ f
l 2., 2• • 4 '.., ,. I 7 .. , . "" 9
10 11 ., 11. 12 11 14.., 14. 15 11 17"" 11• 11 19 to., to• 21 12
n "' n• 24 ,_. 1 2., 2• I 4 '., ,. I 7 . ., •• • 10
11 ., 11 • 12 11 14 "' 14 .. 15 11 17., 17• 11 19 to .. »• 21 21 u., 21• 24
l.P: < 2-11> •i1 .._ <14-11> •i• .._ < 2-U> •ii ...... IOI!: < 2-11> ei1 ...... <14-11> ai1
< 2-21> •i1 ......
~ ftlfJO "'".!!. DSOI07:oM·~ ~ lr:#JO ~ l/IO':m -•ii -'or ooit -'or • i i ..Wr • ii •"4r ~ 0.0200 0.0151
0 .02$7 0,0190 0.024a 0.017' 0.0217 0 .015& 0.0191 O.Ollil o .02Ja 0 .0112 0.0221 o.01n o .o:zoa 0.0160 o .om 0.0151 ~ 0.018' 0.0151 ~ 0.0111 0 .0151
0 .0258 0.0190 0.02M 0.017' 0 ,0210 0 .015& 0.0184 O.Ollil o .oua 0 .0112 0.021• o.om 0.0191 0 .0160 0 .0184 o.om ~ 0.0119 0.0151 ~ 0.0190 o .om
0.0288 0.0190 0.02'9 0.0176 0.02'4 0.0161 0.0219 0.0151 o.0267 0.0112 0.0247 o.om 0 .02.52 0 .0160 o.0219 o.om ~ 0.0204 0.0151 ~ 0.0200 0 .0161
0.0251 0 .0190 O.OU2 0 .0176 0.0208 0.0111 0.0114 0 .0151 o.OZM 0 .0112 o.02u o .om o .01u 0.01&0 0.0184 o .om ~ 0.0171 0.0151 ~ 0.0181 0.0151
0.0271 0 .0190 0 .0249 0.017' 0. ()221 0.0111 0.0191 0.0151 0.02&0 0 .0112 o.ouo o.01n 0 .0211 0 .01&0 0 .0191 o .om ~ 0 .0197 0.0161 ~ 0 ,0QOi 0.0151
0.0211 0 .0190 0.0265 0.017' 0.0240 0.0111 0 .0212 0.0151 o.02&1 0.01112 0.0244 o.om o.0227 0.0110 0.0212 0.0151 ~ 0.0227 0.0151 ~ 0 .0242 0 .0151
o .oa11 0 .0190 O.Oft7 0.0111 o.0274 0 .0161 o .0249 o.om o .0296 0 .01112 o .otN o.01n o .02A o.01eo 0 .020 0 .0161 ~ 0.0228 0.0151 ~ 0.0219 0.0151
0.0291 0 .0190 0.0267 0.017' 0 .02'1 0.0111 0.0211 0 .0151 O.OMZ 0 .01112 0.0242 0.0171 0 .0227 0 .0190 O.Olll 0 .0151 ~ 0.0222 0.0151
8000 1000 l r:#JO 12000 ooil--or ooil~r aoil-•ot.or ooi l-•ot..r
0 .0049 0.0077 O.OOl7 0.0064 0 .0040
S(W)
21i." 24.IO
0 .0061 0.0060 0 .0041 lOOOOOOOC lOOOOOOOC
O.OOll O.OOll 0.0061 0.004&
0.0098 0 .0091 O.OOl5 0 .0076
O.OOll O.OOll 0.0062 0.004&
O.OOll 0 .0071 o.ooee 0.0059
0.0091 o .ocet O.OOl2 0.0071
0.0121 o .om 0.0114 0 .0112
0.0101 0 .0091 O.OOIO 0.0071
0 .0071 O.OOM 0.0011 0 .0017 O.OOl7 o.ooa1 O.OlOI 0 .0094 0.0019 0 .00!0 0.0045 0.0048
O.ODl9 0 .0081 0.0021 0.0022 o.oou O.OOlil
O.OOIO O.OOll 0.0017 0 .0011 O.OOM O.OOll
O.OOll o .cm. 0.0020 0 .002' 0.0041 O.OON
0.0071 0.0086 0.0022 o.oou O.OOM 0 .00N
0.0Da2 O.OOllS
o.0047 o.ooaa o.ooae lOOOOCXXX
O.OOll 0.0089
O.OOll 0.00'8 0.0012 lOOOOOOOC
0.006' 0.0049
o.0046 o.ooaa 0.0017 lOOOOOOOC
0.0027 O.OOl6
O.OOll 0.0047 o.oa&a lOOOOOOOC
O.OC* 0.0064
0.0077 0.0061 0 .0067 lOOOOOOOC
0 .0071 0.0091
0.0111 O.OO'lll 0.0091 lOOOOCXXX
0 .0077 O.ooel
0 .0071 0.00&5 O.OOl7 lOOOOOOOC
0.0057 0 .0017 O.OOll
O.OOl2 0.0020 0 .0048
0.0070 0 .0022 O.OOll
0.0048 0.0017 O.OO&li
0 .0071 0.0019 0 .0045
0 .0059 0.0021 O.OOll
<1-t4> eig .......
0 .0071
0.0044 0.0017 O.OOl6
O.ooel O.OOl!2 0.0051
O.OOM 0.0022 O.OOll
ill.I.. 0 .006' 0.0020 0.0071
22.90 21.67 21.07
lOOOOCOO( U .ti 24.11 29.22
lOOOOOCO( 2'.59 25." U.07
)()()()()()()0( 22.02 u.a 25.51
)()()()()()()()
IS.M • .71 fl.99
lOOOOOOCX I0.11 II.fl' M.IO
lOOOOOOCX I0.11 29.21 21.70
lOOOOOOOC 29.71i
s\r
11.I 9,0
lOOOOOOOC 7.7 ••• 7.4
lOOOOOOCX I.I 1.9
14.4 lOOOOOOOC
12.2 11,0 1.2
lOCOOOOCX 7 .4 I .I
10.6 XXIOOOOOC
10.4 12.4 11.1
lOOOOOOCX 15.4 17.5 11.1
lOCOOOOCX li.5 u .o U .4
lOOOOOOCX U.1
C:.i If D lla9f OS1*17A 1/4 IM D 0.w 1/2/90 ,_ f - IOOO - - IOOO - - 10000 - - 12000 -
•ii ...Wr 0011 met.or •11 ..Wr ooil -.r 1 ~ 0.'1'1'17 0.9975 I ., 1.0049 1.0000 t.OOll 0."91 1.0021 0 ."'4 1.000I 0.9975 1 • 1.ooas o.9'1'16 s.0022 o. 'l'll7 1.0010 o .9911 1.oooa o.9975 I ~ 1.0006 0.9975 4 ~ 1.0002 0.9975 s., 1.0065 1.0000 1.00ll 0.9991 1.0024 0."'4 1.1)001 0.9975 I• 1.0041 0.9991 1.0027 O.'l'll7 1.0011 0.9911 1.000I 0.9975 I XIOOOCIOOOOOOOOOOOOOOOCOOXWlOOOOOllOOOOOOO 1.0010 0. '9975 7 ~ 1.0011 0.9975 I ., 1.0046 1.0000 1.0029 0.9991 1.0011 0."'4 0.9998 0.9975 I • 1.00ll 0.9991 1.0011 0."'7 1.0007 0 .9911 0.'1'1'11 0.9975 t XIOOOCOOOOOOOOO~ 0.9'1'16 o .91J75
10 ~ 1.000I 0.91J75 11 .. 1.00'1 l.0000 1.0042 0.9991 1.0028 0."'4 1.0011 0.'9975 11 ... 1.00« 0,9991 1.0029 0."'7 1.0019 0.9911 1.0011 0.9'175 12 ~ 1.0009 0.9975 11 ~ 0.9988 0.9'175 u ., 1.00l'I 1.0000 1.ooza o.9'192 1.0001 o.9985 o.9991 o.9'171 14 • 1.ocm o.99'17 1.0001 o.99119 o.'1998 o.9912 o.9991 o.9'171 15 lOOCOOOCOOOOOC<·~ 0.9991 0.9'171 11 )'~()( 0.9992 0.9'171 17 .. 1.00ll 1.0000 1.0022 0 .9992 1.0005 0.9'186 0.9918 0.9'7' 17 • 1.0021 0.9991 1.0005 0 .99119 0.9991 0.998t 0.9919 0.9'171 11 ~ 0.9946 0.9'171 lt ~ 1.000& 0.9911 IO "" t.0060 1.0000 1.00ll 0.9991 1.0019 0.9914 1.0001 0.9911 IO• 1.oo&4 0.9997 1.0020 0.99119 1.0009 0 .998t 1.0001 0.9'7' n ~ 1.0004 o.9971 II ~ 1.0004 0.9971 • ... 1.00M 1.0000 1.00ll 0.9"1 1.0025 0.9914 1.0006 0 .9971 a• l .OOM 0.9997 1.0025 0 .99119 1 .0014 0 .9912 1.0006 o.9971 M ~ 0.9991 0.9'71 ,_ f IOOO IOOO 10000 12000
•il-..\or eoi 1-Wr ooi 1-.tor •ii-st.or 0.0022 0.0028
S(XoO)
11.71 as.211
1 I"" 1• I 4 I" s• I
0.0049 0.0040
0.0055 0.0046
0.0042 O.OOli
0 .0047 O.OOtO
o.ooe1 0.0029
0.0040 O.OOli
lOOOOOOO( o.ooao 0.0027 o.ooaa
lOOOOOOO( as.11 15.01 11.61
7 I., 1• • 10
11., 11 • 11 11 14 .. 14• 11 11 17., 17 • 11 lt .... •• 11 22 .... •• M
l.P: < 2-U> •it ._ <14-tl> •i1 ._ < 2-11> •i1 ._ DIJlll: < 2-11) •it ,.. <14-D> •i1
< 1-D> •it ._
0.0046 O.ooa&
O.OOll 0.0048
O.OOM o.oots
O.OOll o.ooa
0.0060 o.ooa1
O.OOM 0.()()41
o.oou 0.0007 0.0011
0.0047 0.0010 o.om O.OOIO 0.0009 o.oou
0.0041 o.oooe 0.0011
o.ooez 0 .0009 0.0019
O.OOl7 0.0009 0 .0025
O.OOll o.ooa1
0.0051 0.0041
o.ooao 0.0011
0.0041 o.ooa1
0.0047 O.OOM
0.0045 O.OOOI 0.0011
O.OOll O.OOOI 0 .0017
0.0041 O.OOOI 0.0021
O.OOl7 0.0005 0 .0011
D.OOll 0.0010 O.OOIO
O. OOll 0.0009 0 .0021
O.OOll 0.0021
0.00« O.OOll
0 .0022 0.0011
0.0020 0.0014
O.OOli o.ooa
0.0041 O.OOIZ
O.OOll 0.0005 0.0011
O.OOIO 0.0010 o.oou
O.OOM 0.0009 0.0024
0.00&2 0.0005 0.0012
0.00!2 0.0009 0.0011
0.00!7 O.OOOI 0.0024
<1-14> • i1 .....
lOOOOOOO(
O.OOM 0.00M 0.0021
lOOOOOOO( 0.0020 o.ooaa O.OOM
lOOOOCXXX O.OOl4 0.0008 0 .0011;
lOOOOOOO( O.aott 0.0011 0.0012
xxxxxxxx 0.0019 0.0027 0.0025
lOOCOOCCX 0.0028 0.0021 o.ooao
lOOOOCXXX 0.0020
o.ooao O.OOOI 0.0011
0 .0021 O.OOOI 0.0011
0.0025 0.0008 0 .0024
IU. 0.0025 O.OOOI 0.0021
lOOOOCCXX 17.01 17.26 14.01
lOOOOCCXX 11.211 11.51 17.2'
lOOOOCCXX • • 71 I0.25 12.01
lOOOOOOCX 11.71 12.211 11.25
lOOOOCCXX U.01 as.01 14.51
lOOOOCCXX 15.lll as.211 as.n
lOOOOCCXX 11.26
11\r •"I st.r (outer)
11.0 12.1 11.1 18.9
lOlOOOOOOOOOOCO 14.1 14.1 11.1 11.1 14.t 11.0 ~
14.1 11.9 15.5 11.4 12.9 11.1
lOOOOOOCIOCOCOC 12.7 11.1 15.I 11.1 11.1 11.4
XIOOOOOOOCCXIOO 11.0 12.1 9.6
10.1 lOOOOOOO(
12.5 11.7 10.1
lOOOOCCXX 11 .1 12.1 11.t
lOOOOCCXX 11.5 11.I 14.0
lOOOOOOO( 11.S
' . .
C.ilf ..... 1 2 ., 2 dn I 4 5 ., 5 dn
• 7 . .., • dn 9
10 11"' 11 ... 12 11 14"' 14 dn 15 11 17., 11• 11 19 20., to• 21 22 u ., n• 24 Peet
1 1., 1• I 4 '., ,. • 7 .. , •• • 10
11 ., 11• l2 11 14., 14• ll 11 17"' 17• 11 1• 20., IO <In 11 22 u., n• 14
IP: ( 1-11> •i1 ...... <14-D> •i1
"• < t-D> .;, " ...
<14-D> .;,
aG7 ""8f OSOI07A 1/4 IM 0 Diiie l/&/9fJ - llOOO - - 9000 - - 10000 - - 12000 -
ooil •nor •ii •™• ooi1 •-'•• •il •llWr ~ 0.9991 0.9974
1.004& 1.0000 1.00M 0.9991 1.0012 0.9984 0.99'16 0.9974 1.0027 0.9994 1.0014 O.'Ml 1.0004 0.9990 0.99'16 0.9'174 ~ 1.0001 0.9'174 ~ 0 .9991 0 .9974
1.0042 1.0000 1.0026 0. '19'11 1.0010 0.9984 0 .99'14 0.9975 1.002' 0.9'194 1.0012 O. 'M7 1.0001 0 .9911 0.99'14 0.9975
lOCIOOOOOOOOOOO:lltOCOO•O»OOOOOOOO( 0 .99'17 0.9975 lOOOOOOOCOOlOOCIOOOIXmCOOOOOOOOOCIXOOO:XOOXOOXX O. 999'1 0. 9'176
1.0017 1.0000 1.0021 0 .'19'11 1.0004 0 .9914 0 .9987 0 .9975 1.0021 0.9991 1.000I 0.99111 0.99'14 0 .9911 0 .99e7 0 .9975
lOCiOOOOOOOCOOO 0 .99el 0.9975 lOCiOOOOOOOCOOO 0.99'14 0.9975
1.00Y 1.0000 1.ooa1 o.mi 1.oou o.9914 1.0001 o .9975 1.00. 0.'991 1.0026 0.99111 1.0015 0.99e1 1.0006 0.9976 ~ 1.0004 0.9975 ~ 0 .998'1 0.9975
1.0046 1.0000 1.C021 0.9991 1.0011 0.9914 0.9991 0.9975 1.ooao o. '991 1.0015 o.9919 1.0004 o.9982 o.9991 o .9975 ~ 1.0002 0.9975 ~ 0.9'191 0 .9975
1.00U 1.0000 l.OOM 0 .9991 1.0020 0.9914 1.000I 0.9975 1.0017 0 .9991 1.002.I 0 .9919 1.0011 0 .9982 1.oooa 0.9975 ~ 1.0008 0.9971 ~ 1.0021 0.9971
1.00U 1.0000 1.0041 0 .99'12 1.0029 0.9986 1.0011 0.997li 1.0047 0 .9991 1 .00ll 0 .9919 1.0021 0.9982 1.0012 0.9975
lOCOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOu~ ('OO()C()()()O( 1.0014 0. 9975 lOOOOOilOOOOOOO 1.0011 0.9975
t .0085 1.0000 l.0046 o. t992 1.ooa1 o. 9986 i.oou o. 9975 1.0049 0.9991 1.00&4 0.9919 1.0024 0.9982 1.0016 0.9975
lOOOOOilOOOOOOO 0.999'1 0.9975 llOOO 9000 10000 12000
•il....t.r •ll- •.Wr •il--r CDi l -•ner 0 .0017
0.0041 O.ooti 0.0028 0.0022 11.ll 12.11
o.ooaa O.OOZ7 0 .0024
0.0041 0 .00&4 0 .0028
lOOOOOOO( 0.0027 0.0021 0 .0019
lOOOOOOO( U .50 12.09 11.11
o.oou 0.0025
o.ooa1 o.ooao O.OOllli 0.0017
o.oca 0.0045 0.0042 O.OOl7
o.oou 0.00411 0 .0041 0.00&4
o.oou 0 .0061 0.0061 0 .0042
0.0065 0 .0061 O.OO&a 0 .0045
0 .0045 O.OON 0 .0008 O.OOOI 0.0019 0 .0016
O.OOIO o.~ 0.0007 0.0006 0.0011 0.0010
O.OOK 0.0041 0.0011 0.0009 0.0019 0 .0016
o.ooaa 0 .0027 0 .0007 0.0008 0.0017 0.0020
O.OCMI 0.0040 O.OOOI O.OOOI 0.0012 0 .0011
0.0041 o.oou 0.0010 0.0010 0.0017 0.0020
0.0020
0.0020 0.0011
0.0089 0.00&4
O.OOM 0.0029
0.0044 0.0089
0.0041 11.0042
0.00211 0 .0008 0 .0019
0.0042 0.0005 0.0010
o.ooas 0.0010 0.0022
O.OOD O.C009 0 .0021
G.OOl7 0.0007 0.0011
O.OOIO 0.0010 0.0021
lOOOOOOO( 0.0022 0 .0024 0 .0012
lOOOOOOO( 0 .0011 0 .0019 o.ooa1
JOOOOOOO( 0 .0029 0 .0014 0 .0021
lOOOOOOO( 0 .0027 0 .0018 O.C021
lOOOOOOO( o.ooaz 0.0046 o.ooa7
lOOOOOOO( o.oora O.OOll 0.0040
lOOOOOOO( 0.001!4
0 .0021 O.OOOI 0.0019
o.oon 0 .0009 0 .0019
O.OOll 0.0009 0.0019
llU.. 0 .002' 0.0009 O.OOM
lOOOOOCCX 12.1& n .eo 29.99
lOOOOOCICX 29.71 11.61 14.41
lOOOOOCICX ..... I0.46 &2.09
lOOOOOCICX aa.50 at .M a .n
lOOOOOCICX .... 17.70 Iii.•
lOOOOOCICX 11.ao a.ea •.51
lOOOOOCICX 12.80
U.1711
""" 11.7 12.0
lOOOOOllOC 11.2 11.7 10.1
lOOOOOllOC 11.4 12.5 10.1
lOOOOOllOC 10.1 11.1 14.1
lOOOOOllOC 14.1 11. 1 12.1
lOOOOOllOC 11.7 12.t 14.0
lOOOOOllOC 14.4 11.1 15.0
lOOOOOllOC 15.9 15.1 11.2
lOOOOOllOC 11.4
11.1444
C.ill Slii•: .,._ 104 MaefOSOI07A 1/4 l.c LI
o.ooa Co 11 .. .,,.,., o IOOO 8000 10000 12000
eizt 0.0106 O.OOl9 O.OOll 0.0012
li•ur fi\ nr- • f(•in) a(O) • 24.12 k,.i J./u • -1.•17 k,.i/•il
ooll1re4 otroa• 9.1
C.ilf Slii•:
ftr•• eizt
106 llogfOSOI07A 1/4 loc UI o.ooa Col ler orrar: o toOO 8000 10000 12000
0.0119 0.0111 0.0100 O.OOll
liftur fl\ et.rue • f(•izt) •(0) • f1 .:rs .,.; "'''" • •l.75' ... i/•11
.. 11 ... .i nr•• 12.1
Coi lf Sloia: .... _ eizt
IOI llotfOSOI07A 1/4 loc O. OOI C.l lor orrar: -0.0015
IOOO 8000 10000 12000 0.0115 O.OlOI 0.0099 0.0090
a
llooor fj\ RrH• • f(• izt) •fO) • 14.11 k,.i iof4r • -2.501 k,.i/•ll
•I trtd .tr-11.0
C.ilf Shi•:
ft.rt• eiz•
I07 MltfOSOIOlA 1/4 lac O.OOI Coller orrar: -0.0015
IOOO 8000 10000 12000 0.0117 0.0108 0 .0100 0.0091
D
liooor f i\ W•" • f(eizt) •fO) • N.al k,.i J./u • · 1.U7 k,.i/•il
.. 1 ... , ....... 1&.1
D•t.t 1/tt0/'1J
D•k 1/lll/'1J
D1\1 l/l/'1J
Coll1r oo,.li•••• Cio kr• of ....... i•••,...kr eoil .tr-) Collor vonin l offM\ (inclivldvol •lier "11¥ f,... • .,.\ coot.tr) u.1• • 0.51 •il•flc,.i 1(0) • 2 .; 1.
Ceil , • .,.,. e\ru• • f(eollor dofloct.i•l •(O) • -a.57 .,.; .,. • 1.785 ... i/•il
An,..._ of 4 •lie: •(O) • I0.00 k,.i de/di • •2.10 k,.i/ai I
C.ller voninl ...it .. : • ••• 11.
A .. ,.... iooor nru• • 10.1 Avor ... °""' .tr- • 11.1
A .. ,.... ~ .. i I nr- • 11.1
CC?l ~M CA-V l iY
C.ilf Slli•:
.tr•• eiz1
104 Moef0$0807A 1/4 loc U o.ooa C.l l1r error: -0.007
eooo 8000 10000 i2000 0.00&6 0.0019 0.0011 0.0002
Ii"" fi\ et.ran • f(•izt) •CO) • 12.10 kpai •Id• • -1.817 kpai/•il
oollond et.rue
••• C.ilf
Sllie: 8'.r••
.1 ..
106 MatfOSOI07A 1/4 loc ut o.ooa Collar error: -0.007 eooo 8000 10000 12000
0.0049 0.0041 O.OOIO 0.0011
liaur fi\ e\ro• • f(eiu) •(0) • 14.'li .,.; ., .... -1.751 .,.i/•il
aollorod ot.n" 1.4
Coi If IOI MtllfOSOI07A 1/4 loc 0 Shi•: O.OCI C.l lar orror: -0.0085
-'"" eooo 8000 10000 12000 eiu o.0046 o.ooae 0.0029 0.0020
liooar f1' ot.rH• • f(eiz•) e(O) • 17 .10 k,.i •/dx • -2.&ol k,. i/ei I
aolfarod .t.ro" 5.0
C.i If I07 lbvfOSOI07A 1/4 loc 0 Shi•: O.OCI Co llor error: -0.0085
-'"" IOOO 1000 10000 12000 eiu 0.0047 o.ooaa O.OOIO 0.0021
linu• fi\ et.re .. • f(ebo) •10) • 11. 'li kpoi •lh. • -2.117 kpoi/ei I
aol orodot.n•
'·'
O.h 1/I0/90
O.\t l/I0/90
01\0 1/1/90
C.llar -Ii•••• Cin \tr• of ntraoo inot.-u\or ooil ot.r••) Collar "r\i<1I oftoo\ (iocliYiddl •liar n11 froa -·' c .. \er) ir./• • O.SI •i l1fkpei 1(0) • 2 •i le
Coi I n•roeo It.rt"• f(oollor dofloc\ion) •(0) • -a.57 kpai .,... • 1.785 .,.i/•il
An._ .,f 4 ooile: e(O) • 15.21 kp11i •fd• • -2. 10 k,.i/•i I
Col lor vor\ie1I ndi .. : 4.1 •ii•
A,yt,.... '""" n,,... 4.t Ann• out.tr ltr•• • 5.1
Anr• ooi I It.re• • 6.1
I .5 =!-- k I£,$ ou:-R...s , ~f'
TASK FORCE DISTRIBUTION:
Roger Bossert (FNAL) Don Capone (SSO..) J. Carson (FNAL) Roger Coombes (SSCL) Dave Fortunato (SSCL) Carl Goochcit (SSO..) Ramesh Gupta (BNL) Jay Jayakumar (SSO..) Paul Mantsch (FNAL) Mike McAshan (SSO..) G. Morgan (BNL) Dave Orrell (SSO..) Bob Palmer (SSCL) Phil Sanger (SSCL) Ron Scanlan (LBL) Robert Schermer (LBL) Giancarlo Spigo (SSCL) Rae Stiening (SSCL) Jim Strait (FNAL) _ Clyde Taylor (LBL) Peter Wanderer (BNL) Erich Willen (BNL) Jon Zabasnik (SSCL)
Magnet Systems Division Business Management Group
MEMORANDUM
To: R. Briggs and T. Bush
From: R.B. Palmer
Date: March 26, 1990
Superconducting Super Collider Laboratory 2550 Bedky~ade Avenue, Suite 220
Dallas, TX 75237·3946
Subject: MAGNET TASK FORCE, INTERIM REPORT #3
This report reflects discussion of the Task Force at its meeting on 3{21/90, held at SSCL, and other discussions.
Modification to preyjous recommendatjop
The recommendation (1) in report #l on the od yoke (13 in.) should be modified to define the OD of the shell. The OD of the shell should be 13-3/8 in. or 340 mm.
Recommendations;
1) the ratio of copper to superconductor for the cables should be:
inner: 1.5: 1 outer: 1.7:1
These choices give: short sample field, field margin, and copper current densities at 6.6 and 7 .2 Tesla of:
inner: 7 .26 T 10% 712 A/mm sq
outer: 7.46T 13% 866A/mm sq
782A/mmsq
953Nmmsq
The copper current densities in the outer cable are higher than some of us would like, but the obsel"Ved rarity of training quench in the outer layer, in current SSC magnets, suggests that this should not be a problem.
In addition, the development of an ·outer cable with ratio of 2.0 : 1 (which would have matched the margins in inner and outer layers) was considered to be a significant task, and not worth the possible small improvement in fll'St quench field
'• .~ .
The cost savings in further raising the copper ratio (eg about S m$ for a change from 1.5: 1 to 1.7: 1) were not considered to be worth the loss in field margin.
Note that this field margin of 10% will probably be reduced by subsequent decisions (see, for instance, recommendation #3).
2) An intermediate temperature Beam Tube Liner should be inserted within the bore of the magnet Cooling, at around 20 degrees. should have the potential capacity of removing at least 10 times the present design synchrotron radiation loss.
Such a liner will allow future upgrades of machine luminosity, by allowing an order of magnitude higher currents.
Such a liner will also allow operation of the magnets at lower than design temperature, this increasing either the operating field or operating margin.
If such a liner is not designed in at this time, it will be either impossible, or very expensive to retrofit it later.
A study of the design of lhi:s bore tube liner should be initiated, at once, jointly by the magnet and accelerator departments.
3) The quadrupole aperture should be raised to S cm
The change will make it possible to insert, within the bore of the quadrupoles (as is now possible in the dipoles), the intermediate temperature beam tube liner.
It will reduce the contributions to field errors from the quadrupoles and make the contribution per meter, or per magnet end, approximately the same as those from the dipoles. Note that the effects on aperture, per meter, or per magnet end, will still be greater for the quadrupoles than for the dipoles, because the beta functions are at their maxima in the quads.
The change will ease the possible problems in winding the pole turns with the wide cable.
The change will make the tooling radii the same for quadrupoles and dipoles. It will also ease the design of interconnects between quadrupoles and dipoles.
4) The new quadrupole design should use the same cable as specified for the outer layer of the dipole. The iron yoke should be allowed to come relatively close to the coil, in order to maximize the gradient and match; as nearly as possible, the droop in the transfer function of the dipole. The field margin should not be less than that in the dipole inner (now 10%) at operating energy.
It is recognized that the resulting quadrupole will have a somewhat lower gradient than that of the present 4 cm design. It will, as a result, have to be somewhat longer. The dipoles will have to be a little (perhaps of the order of 1 % ) shorter, and will have to operate at a sightly higher field. This, in view of the current design field margin, seems reasonable.
5) A priority engineering study is needed on the vertically split yoke design. In order to specify the shell thickness, and thus yoke outside diameter, the loss of stress in the shell during cool down must be calculated. The differential coefficients of expansion and the changing yield strength of the aluminum must be tracked with temperature, and, the effects of friction between the shell and yoke must be included. It might be useful to construct and instrumented short section to observe the behavior of this design.
It is recognized that calculations on the fast track horizontal split yoke must have the highest priority, in as far as they may effect the yoke or collar specifications. But studies on that design, beyond those required for the specification, should give way to those needed for the vertically split yoke.\
6) For the moment, all S cm magnets should use kapton and epoxy fiberglass insulation (the standard insulation).
Nevertheless, the BNL studies of alternatives should be continued, and FNAL should try, within reason, to make their tooling capable of using them.
7) In order to allow continuing study of alternatives (all kapton insulation, aluminum bar yoke, aluminum collars etc.), and to have a real horizontally split yoke, BNL end, backup design; the BNL program should be expanded to include full length 5 cm magnets.
The FNAL program will be hard pressed to produce the required magnets for the string test, and does not have the capability to simultaneously pursue possible serious improvements.
If the alternatives are not pursued actively, and with full length magnets, it will not be possible to incorporated them without significant later delay. To try and pursue these alternatives only in industry, or at SSCL, will be too late, and will lack the BNL experience.
If problems should arise in the FNAL magnets, due to any of the changes that they are introducing, a serious delay will be introduced wtless we have a real, and tested, backup. For FNAL not to adopt these changes, because there is no backup, would mean accepting serious compromises.
We need, and will continue to need, all the expertise we can get. The BNL group has built all the currently tested full length 4 cm coils and associated yokes. They have their 5 cm work to short magnets will greatly reduce their overall involvement and commitment, and limit our access to their expertise.
Recommended Studies
1) Study of the aluminum collar, aluminum bar, vertically split iron yoke, should continue with relatively high priority. This is a very attractive possibility, but will have to be rapidly developed if it is to be available for use in time. The magnetic design of the yoke is being studied at BNL. If a reasonable solution is found, then a stress analysis should be done as soon as possible. This has less priority than that needed for the BNL or FNAL track specifications, but a higher priority than analysis of those designs, after they are specified.
2)Studies (already in progress at BNL and LBL) of alternative methods of correcting the saturation sextupole (with holes, shims. elliptical or other yoke shapes should also continue).
3) Study of the fishbone an and quench venting problem should continue, but this does not now seem to be a high priority question.
4) Studies should also continue of alternative coil arrangements to lower peak fields, simplify construction, and have wedge in the inner layer opposite the pole shim of the outer layer. But these too can continue with relatively low priority. They can be incorporated with little penurbation at a later time.
Subjects For Next Task Force ;
slip planes, teflon and shoes.
End questions: iron, clamping, splice, spacers, interconnects etc.
Review of ongoing studies
Future Meetines;
April 10, 1990
May3, 1990
May9-10, 1990
bl
atSSCL
atLBL
atSSCL
AFD:b.palmer/f.F.report 3
10:00 am to 6:00 pm
9:00 am to 4:00 pm
Building 1. Suite 285