perturbation of vacuum magnetic fields in w7x due to construction errors
DESCRIPTION
Perturbation of vacuum magnetic fields in W7X due to construction errors. T. Andeeva Y. Igitkhanov J. Kisslinger. Outline:. Introduction concerning the generation of magnetic islands Sensitivity of the magnetic configuration with iota=1 Asymmetric target loads due to error fields - PowerPoint PPT PresentationTRANSCRIPT
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Perturbation of vacuum magnetic fields in W7X due to construction errors
Outline:
• Introduction concerning the generation of magnetic islands
• Sensitivity of the magnetic configuration with iota=1
• Asymmetric target loads due to error fields
• Impact of the perturbation fields on high and low iota case
• Effect of coil shift
• Effect of coil declination• Conclusion
T. Andeeva Y. Igitkhanov J. Kisslinger
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Johann Kißlinger
• inexact coil shape
• positioning errors during assembly (shift and declination)
Four assembly steps
• coil imbedding • half module assembly• module assembly• device integration
Construction error possibilities
The construction errors produce symmetry breaking perturbations.
• introduce new island at any periodicity
• modify existing islands• generate and enhance stochastic regions
Perturbations due to inexact coil shape and positioning errors of single coils: Dr. Andreeva’s talk.
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Johann Kißlinger
target
Island geometry
x-point
reso
nant
radi
al fi
eld
ri ~ √ (bmn/('*m))
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Johann Kißlinger
cross-section #cross-section #
Difference of deviation aab14-aab17
Simulation of deviation with different wave length
nlen = 3
nlen = 5nlen = 1
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Johann Kißlinger
Sensitivity of the system
Perturbation by declination of modular coils of 0.02° along a helical axis with m=1
resonant fourier component B11/Bo 1.7*10- 4 , average displacement 0.28mm, max. displacement 0.55mm
= 0°
= 36°
= 72°
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Johann Kißlinger
Perturbation with mainly B22 field component
lateral and radial deviation of up to 7 mm
data set: dl07 ds07 l5 s07
B11/Bo 0.3*10- 4 , B22/Bo 1.9*10- 4
deviation: average 3.6mm
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Johann Kißlinger
Statistical declination of whole modules up to 0.1°
= 0°
= 180°
This specific distribution: B11/Bo 2.3*10- 4 , deviation: average max. 2.3 7.4mm
30 different distributions: fourier coef. B11 B22 B33 B44
average 1.9 0.5 0.3 0.1 max. value 4.4 1.0 0.6 0.2 average dev. 3.4 mm
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Johann Kißlinger
Statistical declination of whole modules up to 0.1°
= 0°
B11/Bo 2.3*10- 4
B11/Bo 1.7*10- 4
declination of modular coils of 0.02° along a helical axis
= 180°
first contact with target
9Johann Kißlinger magnetic field perturbation
period 1
period 2
period 3
period 4
period 5
top target bottom targets
each field period is statistically rotated by 0.1° (3 axis).
Footprints on targets with perturbed field, standard case
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Johann Kißlinger
Statistical shift of whole modules up to 3mm
10 different distributions: fourier coef. B11 B22 B33 B44
average 0.5 0.6 0.2 0.1 max. value 1.1 1.2 0.35 0.15 average dev. 1.75 mm
This specific distribution: B11/Bo 1.1*10- 4 , deviation: average 2.5 max. 3mm
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Johann Kißlinger
high iota standard case low iota
Equal perturbation have different influences at different iota values
FP 2 FP3
x ≈ R* Bmn /(( - r)*m)
with - r >>' x
12Johann Kißlinger magnetic field perturbation
period 1
period 2
period 3
period 4
period 5
each field period is statistically rotated by 0.1° (3 axis).
Footprints on targets with perturbed field, high iota
bottom targetstop targets
13Johann Kißlinger magnetic field perturbation
period 1
period 2
period 3
period 4
period 5
each field period is statistically rotated by 0.1° (3 axis).
Footprints on targets with perturbed field, low iota
bottom targetstop targets
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Johann Kißlinger
Partly compensation of the field component B11
by use of the control coils with individual currents
FP1 2 3 4 5Currents in control coils top 10 -15 -18 0.0 25 kA bottom 0.0 25 10 -15 -18 kA
Field perturbation by statistical declination of 0.1° around 3 axis of whole periods, no compensation
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Compensation by a constant horizontal magnetic field
Field perturbation by statistical declination of 0.1° around 3 axis of whole periods.Compensation of B11 component with Bx = 12G.
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Coordinate system for the coils
M´
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Coordinate system for the coils
M´
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T. Andreeva
Assumptions and scheme of modeling
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7 real and 43 simulated coils
AN11 = 1.3G; AN22 = 1.12G
T. Andreeva
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Effect of coil shifts on B
T. Andreeva
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Effect of rotation on B (-varies)
T. Andreeva
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Effect of rotation on B (-varies)
T. Andreeva
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Effect of rotation on B (-varies)
T. Andreeva
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Effect of rotation on B (=)
T. Andreeva
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Effect of shift and rotation on B (degree
T. Andreeva
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Effect of shift and rotation on B (=0.1 degree)
T Andreeva
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Effect of shift and rotation on B (=0.2 degree)
T. Andreeva
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Tamara Andreeva
Effect of shift and rotation on B (=0.3 degree)
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x10-4
B for an average deviation of 1mm caused by different types of coil errors
x10-4
Average perturbation Maximum perturbation
T. Andreeva
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Conclusions:
• Deviations with an average value of 1.5 to 2mm with a statistical distribution may generate effective field perturbations in the range of 2*10-4 given by the proposal.
• Mainly the m=1, n=1 island appears.
• The field perturbation go almost linearly with the amplitude of the deviation.
• Due to the low-order islands the load on the targets is asymmetric.
• In the high iota configuration the centre region is displaced while the edge region is not
so strong influenced.
• The more systematic deviations due to rotation of coils and whole modules is more
effective in producing low order B perturbations then the deviations of coil shape
and shift errors.
• The small scale deviations of the manufacturing errors enhances the stochastic structures at the edge.• The control coils are not very effective for compensating low-order error fields.
Outlook: Continue the calculation in collaboration with the engineering team. Compensation of the low order error fields with the planar coils should be more effective but needs extra current feeders. Consider the possibility of evaluation of scaling law for the magnetic field perturbations.