SLAC Magnetic Measurements
Date: 07-18-1995
Time: 06:18:47

Magnet Name (Serial #): 053
Bar Code Number: 025
Project: PEP II High Energy Ring Sextupoles
Test Stand: IR8, S1, N
Measurement Coil: # 1
Operator: bmd
Run Number: 1
Comment: 

Standardization Currents (A):
   250.0    10.0   200.0    10.0   200.0    10.0   200.0
    10.0

Test Currents (A):
    25.0    50.0   100.0   125.0   150.0   175.0   200.0
   150.0   100.0    50.0    25.0


                 Harmonics Measurements

Date: 07-18-1995
Time: 06:49:05
Magnet Name: 053
Run Number: 1


                          FIELD HARMONICS

Magnet Current, Imag =  25.61969  +-  3.197585E-03  A
Coil Radius, Rcoil =  .044882  m
Coil # Turns, Nturns =  20 
Average, # Rotations/Measurement =  10 , # Measurements =  4 
Nmain =  3 

 N     BLn     sigBLn    THspole   sigTH    BLn/BLN sBLn/BLN
       (Tm)     (Tm)      (deg)    (deg)      (%)      (%)  
---  --------+--------  --------+--------  --------+--------
  1   0.00006  0.00000   -105.67     1.01    1.1369   0.0108
  2   0.00006  0.00000    -84.48     0.37    1.2136   0.0064
  3   0.00526  0.00000     30.11     0.00  100.0000   0.0673
  4   0.00001  0.00000     -7.59     2.58    0.1349   0.0248
  5   0.00001  0.00000    -14.18     3.01    0.1290   0.0120
  6   0.00000  0.00000      6.22     9.02    0.0291   0.0270
  7   0.00000  0.00000     -7.96     4.21    0.0792   0.0136
  8   0.00000  0.00000     -4.74     9.05    0.0343   0.0115
  9   0.00002  0.00000     -9.38     0.47    0.3689   0.0492
 10   0.00000  0.00000     -4.05     9.99    0.0401   0.0189
 11   0.00000  0.00000      0.65     5.49    0.0407   0.0357
 12   0.00000  0.00000     -4.29     7.87    0.0269   0.0076
 13   0.00000  0.00000     -2.14     5.89    0.0246   0.0141
 14   0.00000  0.00000      4.31     4.26    0.0271   0.0149
 15   0.00000  0.00000     -5.50     1.18    0.0884   0.0195
 16   0.00000  0.00000      3.80     3.23    0.0381   0.0242


The magnetic center is at
X =    52.2 +-     3.4 microns
Y =   267.3 +-     1.6 microns

The magnetic center is measured relative to the coil axis
effectively at the longitudinal center of the magnet.
Pitch and yaw are not seen by the coil.

View from the non-lead end of the magnet:

           y          
           ^          
           |          
           N          
        S     S       
                --> x 
        N     N       
           S          

Date: 07-18-1995
Time: 06:52:30
Magnet Name: 053
Run Number: 1


                          FIELD HARMONICS

Magnet Current, Imag =  50.60001  +-  1.507188E-03  A
Coil Radius, Rcoil =  .044882  m
Coil # Turns, Nturns =  20 
Average, # Rotations/Measurement =  10 , # Measurements =  4 
Nmain =  3 

 N     BLn     sigBLn    THspole   sigTH    BLn/BLN sBLn/BLN
       (Tm)     (Tm)      (deg)    (deg)      (%)      (%)  
---  --------+--------  --------+--------  --------+--------
  1   0.00007  0.00000   -102.03     0.40    0.7142   0.0024
  2   0.00012  0.00000    -85.00     0.24    1.2137   0.0021
  3   0.01027  0.00000     30.11     0.00  100.0000   0.0401
  4   0.00001  0.00000     -8.39     1.80    0.1056   0.0057
  5   0.00001  0.00000    -16.65     1.72    0.1358   0.0381
  6   0.00000  0.00000      7.01    13.72    0.0097   0.0046
  7   0.00001  0.00000    -11.96     2.07    0.0499   0.0268
  8   0.00000  0.00000     -0.83     6.92    0.0144   0.0055
  9   0.00003  0.00000    -10.00     0.05    0.3349   0.0082
 10   0.00000  0.00000     -1.22    13.24    0.0228   0.0110
 11   0.00000  0.00000      3.80    12.11    0.0124   0.0045
 12   0.00000  0.00000      3.08    10.92    0.0140   0.0047
 13   0.00000  0.00000     -0.44     8.49    0.0144   0.0053
 14   0.00000  0.00000      5.10     2.20    0.0116   0.0050
 15   0.00001  0.00000     -5.76     0.17    0.0677   0.0021
 16   0.00000  0.00000      4.13     6.07    0.0131   0.0032


The magnetic center is at
X =    47.3 +-     2.3 microns
Y =   268.2 +-     0.6 microns

The magnetic center is measured relative to the coil axis
effectively at the longitudinal center of the magnet.
Pitch and yaw are not seen by the coil.

View from the non-lead end of the magnet:

           y          
           ^          
           |          
           N          
        S     S       
                --> x 
        N     N       
           S          

Date: 07-18-1995
Time: 06:55:59
Magnet Name: 053
Run Number: 1


                          FIELD HARMONICS

Magnet Current, Imag =  100.5946  +-  1.413287E-03  A
Coil Radius, Rcoil =  .044882  m
Coil # Turns, Nturns =  20 
Average, # Rotations/Measurement =  10 , # Measurements =  4 
Nmain =  3 

 N     BLn     sigBLn    THspole   sigTH    BLn/BLN sBLn/BLN
       (Tm)     (Tm)      (deg)    (deg)      (%)      (%)  
---  --------+--------  --------+--------  --------+--------
  1   0.00010  0.00000    -98.99     0.26    0.5008   0.0010
  2   0.00024  0.00000    -85.22     0.04    1.1990   0.0055
  3   0.02039  0.00001     30.10     0.00  100.0000   0.0683
  4   0.00002  0.00000     -7.71     0.44    0.1135   0.0038
  5   0.00002  0.00000    -16.88     1.83    0.0998   0.0241
  6   0.00000  0.00000     18.73    11.38    0.0097   0.0039
  7   0.00001  0.00000      0.89    12.67    0.0259   0.0047
  8   0.00000  0.00000     -0.78     1.73    0.0145   0.0056
  9   0.00007  0.00000     -9.80     0.09    0.3225   0.0053
 10   0.00000  0.00000     -6.95    11.83    0.0073   0.0033
 11   0.00000  0.00000      0.62    10.93    0.0078   0.0014
 12   0.00000  0.00000     -0.39     1.67    0.0067   0.0031
 13   0.00000  0.00000     -7.79     3.39    0.0072   0.0055
 14   0.00000  0.00000     -1.78     0.54    0.0124   0.0045
 15   0.00002  0.00000     -6.09     0.09    0.0785   0.0036
 16   0.00000  0.00000     -2.63     5.71    0.0063   0.0030


The magnetic center is at
X =    44.7 +-     0.4 microns
Y =   265.3 +-     1.2 microns

The magnetic center is measured relative to the coil axis
effectively at the longitudinal center of the magnet.
Pitch and yaw are not seen by the coil.

View from the non-lead end of the magnet:

           y          
           ^          
           |          
           N          
        S     S       
                --> x 
        N     N       
           S          

Date: 07-18-1995
Time: 07:02:42
Magnet Name: 053
Run Number: 1


                          FIELD HARMONICS

Magnet Current, Imag =  150.5742  +-  4.334154E-03  A
Coil Radius, Rcoil =  .044882  m
Coil # Turns, Nturns =  20 
Average, # Rotations/Measurement =  10 , # Measurements =  4 
Nmain =  3 

 N     BLn     sigBLn    THspole   sigTH    BLn/BLN sBLn/BLN
       (Tm)     (Tm)      (deg)    (deg)      (%)      (%)  
---  --------+--------  --------+--------  --------+--------
  1   0.00014  0.00000    -96.51     0.34    0.4449   0.0019
  2   0.00036  0.00000    -85.24     0.04    1.1965   0.0019
  3   0.03045  0.00001     30.11     0.00  100.0000   0.0496
  4   0.00004  0.00000     -7.41     0.39    0.1169   0.0049
  5   0.00004  0.00001    -16.14     1.15    0.1334   0.0259
  6   0.00000  0.00000      3.78     0.46    0.0099   0.0031
  7   0.00001  0.00001    -10.09     2.59    0.0374   0.0176
  8   0.00001  0.00000     -0.24     0.45    0.0186   0.0019
  9   0.00010  0.00000     -9.82     0.05    0.3316   0.0033
 10   0.00000  0.00000      4.03    12.59    0.0024   0.0006
 11   0.00000  0.00000     -3.39     5.18    0.0021   0.0009
 12   0.00000  0.00000      1.55    13.43    0.0052   0.0013
 13   0.00000  0.00000     -6.22     2.92    0.0020   0.0002
 14   0.00000  0.00000     -2.09     1.82    0.0072   0.0011
 15   0.00002  0.00000     -5.86     0.11    0.0690   0.0026
 16   0.00000  0.00000     -3.31     2.78    0.0052   0.0012


The magnetic center is at
X =    44.4 +-     0.4 microns
Y =   264.8 +-     0.4 microns

The magnetic center is measured relative to the coil axis
effectively at the longitudinal center of the magnet.
Pitch and yaw are not seen by the coil.

View from the non-lead end of the magnet:

           y          
           ^          
           |          
           N          
        S     S       
                --> x 
        N     N       
           S          

Date: 07-18-1995
Time: 07:09:25
Magnet Name: 053
Run Number: 1


                          FIELD HARMONICS

Magnet Current, Imag =  200.5696  +-  2.484045E-03  A
Coil Radius, Rcoil =  .044882  m
Coil # Turns, Nturns =  20 
Average, # Rotations/Measurement =  10 , # Measurements =  4 
Nmain =  3 

 N     BLn     sigBLn    THspole   sigTH    BLn/BLN sBLn/BLN
       (Tm)     (Tm)      (deg)    (deg)      (%)      (%)  
---  --------+--------  --------+--------  --------+--------
  1   0.00016  0.00000    -95.79     0.29    0.3948   0.0023
  2   0.00048  0.00000    -85.33     0.03    1.1978   0.0009
  3   0.04045  0.00001     30.11     0.00  100.0000   0.0219
  4   0.00005  0.00000     -7.59     0.44    0.1174   0.0031
  5   0.00005  0.00000    -16.90     1.22    0.1235   0.0101
  6   0.00000  0.00000      2.57     2.30    0.0073   0.0018
  7   0.00001  0.00000    -12.18     3.46    0.0273   0.0106
  8   0.00001  0.00000     -0.72     2.32    0.0159   0.0035
  9   0.00013  0.00000     -9.82     0.02    0.3321   0.0016
 10   0.00000  0.00000     -2.30    13.02    0.0060   0.0024
 11   0.00000  0.00000      0.01     4.21    0.0055   0.0021
 12   0.00000  0.00000      2.67     7.43    0.0023   0.0011
 13   0.00000  0.00000     -1.11     4.75    0.0039   0.0020
 14   0.00000  0.00000     -4.16     4.06    0.0058   0.0021
 15   0.00003  0.00000     -5.82     0.10    0.0720   0.0018
 16   0.00000  0.00000      0.23     9.84    0.0039   0.0028


The magnetic center is at
X =    43.6 +-     0.3 microns
Y =   265.2 +-     0.2 microns

The magnetic center is measured relative to the coil axis
effectively at the longitudinal center of the magnet.
Pitch and yaw are not seen by the coil.

View from the non-lead end of the magnet:

           y          
           ^          
           |          
           N          
        S     S       
                --> x 
        N     N       
           S          


           SUMMARY OF THE CALCULATIONS AND CONVENTIONS USED


Field Expansion:
The expansion of the radial and azimuthal field in polar
coordinates is
 Br(r,th) = Sum Bn (r/rref)^(n-1) cos(n(th-thspole))
 Bth(r,th) = -Sum Bn (r/rref)^(n-1) sin(n(th-thspole))
Our convention is to set rref = Rcoil.
Thspole is the angle of the first magnetic south pole
with respect to the horizontal, measured ccw by a shaft
encoder in the system.

Coil Voltage:
The coil voltage from each field harmonic is
 Vn(th) = Nturns * velocity * Brn(Rcoil,th) * L
L is the magnet effective length, or BLn is the integrated
field strength of the n'th harmonic.
At the coil radius, the radial field as a function of angle is,
 Brn(Rcoil,th) * L = BLn * cos(n*(th - thspole))
The coil voltage is
 Vn(th) = Nturns * velocity * BLn * cos(n*(th - thspole))
        = Nturns * Rcoil * ang_freq * BLn * cos(n*(th - THspole))
An FFT of the coil voltage gives Vn and PhiVn according to the formula
 Vn(i) = Vn * cos(n*2pi*i/N + PhiVn)

Multipole Field Calculations:
To find the multipole field magnitudes and phases,
the measured voltage harmonics are related to their values
calculated from the field harmonics:
 Nturns * Rcoil * ang_freq * BLn = Vn
 -n * thspole = PhiVn
Or,
 BLn = Vn / (Nturns * Rcoil * ang_freq)
 thspole = -PhiVn / n

Harmonic Strength Ratios:
The main field, denoted by capital N, is the field harmonic
with the largest strength at the coil radius.
The field strength ratio is defined by
 Rn = BLn / BLN
It gives the ratio of each harmonic field strength to the
main field strength at the coil radius.

Calculation Of SL:
The sextupole strength S is defined by the vertical
field on the x-axis (median plane).
It is the quadratic term in the Taylor expansion.
 By(x) = 1/2 S x^2
On the x-axis, By(x) = Bth(r=x,th=0)
From the expression for Bth above,
 By(x) = - B3 (x/rref)^2 sin(-3 thspole)
Take rref = Rcoil, thspole = pi/6, then at x=Rcoil,
 By(Rcoil) = B3 = 1/2 S Rcoil^2
So,
 S = 2 B3 / Rcoil^2
The integrated sextupole strength is
 SL = 2 BL3 / Rcoil^2

Calculation Of The Sextupole Center:
In the sextupole's frame,
 Bx' = S * x' * y'
 By' = 1/2 * S * (x'^2 - y'^2).
In the coil's frame (unprimed frame) the magnetic center is at (x0, y0).
In the coil's frame,
 Bx = S * (x - x0) * (y - y0)
 By = 1/2 * S * [(x - x0)^2 - (y - y0)^2].
The magnetic center can be found in terms of the measured
quadrupole field.  Compare Br and Btheta on the x-axis to
 Bxquad = -S * (x0 * y + y0 * x)
 Byquad = -S * (x0 * x - y0 * y).
Evaluate at x = Rcoil, y = 0 and compare to
 Br(theta = 0) = Bx, Btheta(theta = 0) = By.
In terms of the measured integrated strengths, this gives
 Xcenter = x0 = - (1/(SL * Rcoil)) * BL2 * sin(2 * THspole2)
 Ycenter = y0 = - (1/(SL * Rcoil)) * BL2 * cos(2 * THspole2)
