SLAC Magnetic Measurements Date: 09-01-1995 Time: 06:15:39 Magnet Name (Serial #): 090 Bar Code Number: 125 Project: PEP II High Energy Ring Sextupoles Test Stand: IR8, S1, N Measurement Coil: # 1 Operator: dan Run Number: 2 Comment: power supply shut off 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: 09-01-1995 Time: 06:46:03 Magnet Name: 090 Run Number: 2 FIELD HARMONICS Magnet Current, Imag = 25.68637 +- 5.656551E-04 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 -105.81 0.10 1.1240 0.0009 2 0.00004 0.00000 6.62 0.10 0.7684 0.0028 3 0.00527 0.00000 -29.93 0.00 100.0000 0.0649 4 0.00000 0.00000 43.16 0.45 0.0728 0.0025 5 0.00001 0.00000 18.59 0.15 0.1445 0.0009 6 0.00000 0.00000 -27.47 0.99 0.0081 0.0024 7 0.00000 0.00000 14.03 0.23 0.0375 0.0014 8 0.00000 0.00000 -9.80 18.14 0.0090 0.0028 9 0.00002 0.00000 10.10 0.03 0.3303 0.0028 10 0.00000 0.00000 2.60 8.34 0.0034 0.0031 11 0.00000 0.00000 8.60 4.67 0.0080 0.0050 12 0.00000 0.00000 -8.00 6.17 0.0050 0.0014 13 0.00000 0.00000 2.75 7.24 0.0043 0.0032 14 0.00000 0.00000 1.48 7.11 0.0049 0.0009 15 0.00000 0.00000 6.25 0.17 0.0713 0.0057 16 0.00000 0.00000 0.58 2.88 0.0032 0.0021 The magnetic center is at X = 39.5 +- 0.6 microns Y = 167.9 +- 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 N --> x S S N Date: 09-01-1995 Time: 06:49:28 Magnet Name: 090 Run Number: 2 FIELD HARMONICS Magnet Current, Imag = 50.66913 +- 2.143139E-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 0.00005 0.00000 -113.14 0.10 0.4702 0.0012 2 0.00008 0.00000 7.36 0.09 0.8002 0.0010 3 0.01028 0.00001 -29.93 0.00 100.0000 0.1405 4 0.00001 0.00000 41.50 0.46 0.0801 0.0017 5 0.00002 0.00000 18.50 0.13 0.1653 0.0014 6 0.00000 0.00000 -11.38 22.95 0.0052 0.0018 7 0.00000 0.00000 13.75 0.21 0.0410 0.0015 8 0.00000 0.00000 -18.88 1.66 0.0101 0.0017 9 0.00003 0.00000 10.11 0.03 0.3323 0.0022 10 0.00000 0.00000 -1.88 4.42 0.0028 0.0018 11 0.00000 0.00000 8.21 6.80 0.0026 0.0009 12 0.00000 0.00000 -1.90 4.94 0.0020 0.0009 13 0.00000 0.00000 5.36 3.85 0.0025 0.0006 14 0.00000 0.00000 10.84 0.97 0.0040 0.0008 15 0.00001 0.00000 6.08 0.06 0.0712 0.0016 16 0.00000 0.00000 3.39 8.48 0.0024 0.0012 The magnetic center is at X = 45.6 +- 0.6 microns Y = 173.7 +- 0.3 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 N --> x S S N Date: 09-01-1995 Time: 06:52:57 Magnet Name: 090 Run Number: 2 FIELD HARMONICS Magnet Current, Imag = 100.6543 +- 9.323951E-04 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 0.00003 0.00000 -141.98 0.50 0.1497 0.0009 2 0.00016 0.00000 7.91 0.02 0.8062 0.0026 3 0.02038 0.00001 -29.93 0.00 100.0000 0.0429 4 0.00002 0.00000 40.64 0.20 0.0886 0.0019 5 0.00004 0.00000 18.46 0.08 0.1717 0.0013 6 0.00000 0.00000 -29.17 0.27 0.0147 0.0009 7 0.00001 0.00000 13.85 0.06 0.0403 0.0015 8 0.00000 0.00000 -19.48 1.05 0.0098 0.0004 9 0.00007 0.00000 10.10 0.03 0.3307 0.0025 10 0.00000 0.00000 12.68 1.48 0.0036 0.0002 11 0.00000 0.00000 3.57 3.72 0.0009 0.0006 12 0.00000 0.00000 0.05 0.49 0.0084 0.0009 13 0.00000 0.00000 4.26 2.75 0.0029 0.0010 14 0.00000 0.00000 -5.94 7.75 0.0028 0.0010 15 0.00001 0.00000 6.05 0.06 0.0728 0.0017 16 0.00000 0.00000 -0.86 1.40 0.0029 0.0010 The magnetic center is at X = 49.3 +- 0.2 microns Y = 174.1 +- 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 N --> x S S N Date: 09-01-1995 Time: 06:59:41 Magnet Name: 090 Run Number: 2 FIELD HARMONICS Magnet Current, Imag = 150.6405 +- 2.688471E-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 0.00003 0.00000 155.89 0.82 0.1039 0.0017 2 0.00025 0.00000 7.74 0.04 0.8104 0.0025 3 0.03046 0.00002 -29.93 0.00 100.0000 0.0793 4 0.00003 0.00000 40.98 0.11 0.0885 0.0021 5 0.00005 0.00000 18.43 0.02 0.1758 0.0008 6 0.00000 0.00000 -26.96 1.04 0.0058 0.0019 7 0.00001 0.00000 13.62 0.17 0.0398 0.0015 8 0.00000 0.00000 -18.28 1.87 0.0080 0.0013 9 0.00010 0.00000 10.06 0.01 0.3312 0.0009 10 0.00000 0.00000 -0.82 5.90 0.0016 0.0004 11 0.00000 0.00000 1.37 4.48 0.0014 0.0008 12 0.00000 0.00000 -0.35 14.14 0.0056 0.0007 13 0.00000 0.00000 -2.01 6.17 0.0027 0.0016 14 0.00000 0.00000 -5.75 8.95 0.0032 0.0012 15 0.00002 0.00000 6.08 0.08 0.0684 0.0013 16 0.00000 0.00000 -0.24 1.72 0.0027 0.0009 The magnetic center is at X = 48.6 +- 0.3 microns Y = 175.3 +- 0.5 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 N --> x S S N Date: 09-01-1995 Time: 07:06:25 Magnet Name: 090 Run Number: 2 FIELD HARMONICS Magnet Current, Imag = 200.6321 +- 6.142871E-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 0.00005 0.00000 133.60 0.41 0.1231 0.0015 2 0.00033 0.00000 7.58 0.06 0.8227 0.0016 3 0.04044 0.00002 -29.93 0.00 100.0000 0.0591 4 0.00004 0.00000 41.15 0.15 0.0969 0.0014 5 0.00007 0.00000 18.34 0.10 0.1756 0.0004 6 0.00000 0.00000 -13.05 24.11 0.0069 0.0006 7 0.00002 0.00000 13.70 0.05 0.0411 0.0013 8 0.00000 0.00000 -9.13 17.46 0.0091 0.0006 9 0.00014 0.00000 10.07 0.05 0.3348 0.0018 10 0.00000 0.00000 1.94 13.08 0.0034 0.0009 11 0.00000 0.00000 -1.71 6.85 0.0019 0.0004 12 0.00000 0.00000 -1.81 7.73 0.0010 0.0005 13 0.00000 0.00000 3.51 2.54 0.0027 0.0024 14 0.00000 0.00000 -3.88 8.03 0.0045 0.0010 15 0.00003 0.00000 6.02 0.15 0.0704 0.0013 16 0.00000 0.00000 -7.52 1.70 0.0020 0.0001 The magnetic center is at X = 48.3 +- 0.4 microns Y = 178.2 +- 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 ^ | S N N --> x S S N 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)