SLAC Magnetic Measurements
Date: 07-16-1997
Time: 16:15:27

Project: PEP2INJ
Magnet Type: QUAD
Magnet Name (Serial #): 2Q4W-11
Bar Code Number: QM31 9380
Test Stand: 1
Measurement System: DC100
Operator: tss
Run Number: 3
Comment: measuring magnet after modifications for intallation into beam line.

Standardization Currents
 3  cycles, 0 to  180  to 0 A

Test Currents
    10.0    30.0    50.0    60.0    70.0    80.0    90.0
   100.0   110.0   120.0   130.0   140.0   150.0   160.0
   180.0   150.0   100.0    50.0


                 Harmonics Measurements

Date: 07-16-1997
Time: 16:36:41
Magnet Name: 2Q4W-11
Run Number: 3


                         FIELD HARMONICS

Magnet Current, Imag =  50.04091  +-  2.991194E-04  A
Harmonics at Rcoil =  .0189973  m
Nmain =  2 

 n     BLn     sigBLn    THspole   sigTH    BLn/BLN sBLn/BLN
       (Tm)     (Tm)      (deg)    (deg)      (%)      (%)  
---  --------+--------  --------+--------  --------+--------
  1   0.00004  0.00000    161.99     0.71    0.2589   0.0057
  2   0.01413  0.00000    -52.58     0.02  100.0000   0.0467
  3   0.00003  0.00000    -28.38     1.84    0.1785   0.0174
  4   0.00007  0.00000    -28.83     0.30    0.4752   0.0058
  5   0.00001  0.00000    -13.57     2.99    0.0635   0.0184
  6   0.00002  0.00001      7.11     2.28    0.1399   0.0357
  7   0.00001  0.00000      7.20    11.84    0.0652   0.0154
  8   0.00001  0.00001     -1.99    15.59    0.0860   0.0418
  9   0.00001  0.00000    -13.83     4.84    0.0487   0.0097
 10   0.00003  0.00000      1.23     0.35    0.2015   0.0063
 11   0.00000  0.00000      6.43     3.14    0.0125   0.0058
 12   0.00000  0.00000      0.16    13.70    0.0135   0.0066
 13   0.00000  0.00000     -1.27     7.59    0.0057   0.0015
 14   0.00001  0.00000     -0.86     0.18    0.0355   0.0035
 15   0.00000  0.00000      4.34     3.23    0.0045   0.0007
 16   0.00000  0.00000      2.65     3.02    0.0052   0.0023


The magnetic center is at
X =    15.2 +-     0.7 microns
Y =   -46.8 +-     1.0 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          
           ^          
           |          
        S     N       

                --> x 

        N     S       

Date: 07-16-1997
Time: 16:55:36
Magnet Name: 2Q4W-11
Run Number: 3


                         FIELD HARMONICS

Magnet Current, Imag =  110.1048  +-  2.617172E-04  A
Harmonics at Rcoil =  .0189973  m
Nmain =  2 

 n     BLn     sigBLn    THspole   sigTH    BLn/BLN sBLn/BLN
       (Tm)     (Tm)      (deg)    (deg)      (%)      (%)  
---  --------+--------  --------+--------  --------+--------
  1   0.00005  0.00000    139.47     1.04    0.1695   0.0054
  2   0.03112  0.00002    -52.61     0.02  100.0000   0.0798
  3   0.00005  0.00000    -28.82     1.13    0.1724   0.0142
  4   0.00015  0.00000    -28.88     0.34    0.4764   0.0034
  5   0.00003  0.00000    -13.03     4.33    0.0818   0.0116
  6   0.00005  0.00001      9.27     2.86    0.1608   0.0250
  7   0.00002  0.00000      6.69    13.43    0.0608   0.0084
  8   0.00003  0.00001      1.93    12.38    0.0918   0.0401
  9   0.00002  0.00001    -12.55     2.87    0.0485   0.0244
 10   0.00006  0.00000      1.80     0.09    0.1863   0.0087
 11   0.00000  0.00000      2.98     7.31    0.0071   0.0048
 12   0.00000  0.00000     10.04     2.06    0.0092   0.0030
 13   0.00000  0.00000     -9.00     2.28    0.0075   0.0020
 14   0.00001  0.00000     -1.34     0.41    0.0356   0.0022
 15   0.00000  0.00000     -0.13     5.91    0.0048   0.0008
 16   0.00000  0.00000     -2.44     2.44    0.0044   0.0017


The magnetic center is at
X =    20.9 +-     0.8 microns
Y =   -24.5 +-     0.9 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          
           ^          
           |          
        S     N       

                --> x 

        N     S       

Date: 07-16-1997
Time: 17:14:46
Magnet Name: 2Q4W-11
Run Number: 3


                         FIELD HARMONICS

Magnet Current, Imag =  169.8847  +-  3.260172E-04  A
Harmonics at Rcoil =  .0189973  m
Nmain =  2 

 n     BLn     sigBLn    THspole   sigTH    BLn/BLN sBLn/BLN
       (Tm)     (Tm)      (deg)    (deg)      (%)      (%)  
---  --------+--------  --------+--------  --------+--------
  1   0.00015  0.00000    106.52     0.65    0.2942   0.0023
  2   0.05071  0.00004    -52.55     0.01  100.0000   0.1188
  3   0.00006  0.00000    -25.63     1.71    0.1276   0.0026
  4   0.00023  0.00001    -28.84     0.15    0.4563   0.0120
  5   0.00004  0.00001    -12.85     4.75    0.0757   0.0191
  6   0.00007  0.00002      8.22     2.55    0.1475   0.0387
  7   0.00004  0.00000      9.73    12.11    0.0758   0.0072
  8   0.00004  0.00002      4.26    13.72    0.0816   0.0424
  9   0.00002  0.00001     -3.33    13.54    0.0490   0.0129
 10   0.00010  0.00000      1.73     0.08    0.2035   0.0061
 11   0.00001  0.00000      4.95     1.88    0.0110   0.0046
 12   0.00000  0.00000     -3.65     5.08    0.0064   0.0019
 13   0.00000  0.00000     -1.28     5.23    0.0024   0.0007
 14   0.00002  0.00000     -0.75     0.23    0.0356   0.0016
 15   0.00000  0.00000      5.31     3.38    0.0037   0.0007
 16   0.00000  0.00000      1.84     3.05    0.0043   0.0016


The magnetic center is at
X =    53.6 +-     0.5 microns
Y =   -15.9 +-     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          
           ^          
           |          
        S     N       

                --> x 

        N     S       


           SUMMARY OF THE CALCULATIONS AND CONVENTIONS USED


Calculation Of GL:
V2 = Nturns * velocity * B2 * L
   = Nturns * Rcoil * ang_freq * GL * Rcoil
   = Nturns * Rcoil^2 * ang_freq * GL
GL = V2 / (Nturns * Rcoil^2 * ang_freq)
For a double coil (for coil bowing correction),
GL = ( (1 / Nturns * Rcoil^2)1 + (1 / Nturns * Rcoil^2)2 ) * (V2 / ang_freq)
Let CoilConst = ( (1 / Nturns * Rcoil^2)1 + (1 / Nturns * Rcoil^2)2 )
GL = CoilConst * V2 / ang_freq


Calculation Of The Harmonics:
Magnitude, harmonic n:
Vn = Nturns * velocity * Bn * L
   = Nturns * Rcoil * ang_freq * (BLn)
BLn = Vn / (Nturns * Rcoil * ang_freq)
Rn = BLn / BL2 = Vn / V2

Phase, harmonic n:
At the coil radius, the radial field as a function of angle is,
BLn(th) = BLn * cos(n*(th - THspole))
The coil voltage Vn(th) = Nturns * velocity * BLn(th)
Vn(th) = Nturns * Rcoil * ang_freq * BLn * cos(n*(th - THspole))
The FFT gives Vn and PhiVn in the formula
Vn(i) = Vn * cos(n*2pi*i/N + PhiVn)
So, Nturns * Rcoil * ang_freq * BLn = Vn
    -n * THspole = PhiVn
Or, BLn = Vn / (Nturns * Rcoil * ang_freq)
    THspole = -PhiVn / n


Calculation Of The Magnetic Center:
In the quadrupole's frame, Bx' = G * y', By' = G * x'.
In the coil's frame (unprimed frame) the magnetic center is at (x0, y0).
In the coil's frame,
     Bx = G * (y - y0), By = G * (x - x0).
This gives the magnetic center in terms of the measured
dipole field.
     x0 = - By / G, y0 = - Bx / G
In terms of the measured integrated strengths,
     Xcenter = - (1/GL) * BL1 * sin(THspole1)
     Ycenter = - (1/GL) * BL1 * cos(THspole1)
