e-Beam Mapping Plans (FY09) - PowerPoint PPT Presentation

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e-Beam Mapping Plans (FY09)

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NCSX will have a few weeks for preliminary e-beam mapping ... Verify correct rotational transform; for example, by locating rational surfaces (using islands) ... – PowerPoint PPT presentation

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Title: e-Beam Mapping Plans (FY09)


1
e-Beam Mapping Plans (FY09)
NCSX
  • E. Fredrickson,
  • For the NCSX Team

Auburn
NCSX Research Forum Dec. 7, 2006
2
Goals of e-beam mapping studies
  • NCSX will have a few weeks for preliminary e-beam
    mapping experiments in FY09.
  • e-beam mapping goals
  • Verify coil assembly accuracy
  • Measure error-field induced islands.
  • Document control of vacuum field characteristics
    with coil currents
  • Document good surfaces over wide range of
    configurations (e.g., iota-scan)
  • Verify correct rotational transform for example,
    by locating rational surfaces (using islands)

3
Auburn will collaborate on e-beam mapping
campaign
  • Auburn is also lending hardware
  • Movable electron gun, camera
  • Help with detection apparatus
  • Evaluating options for detection apparatus
  • Wire mesh
  • Sparse, jogged mesh
  • Fluorescent rod
  • Additional issues under study
  • Field value/pulse length (2 kG gt 30s, 1 kG gt2
    min)
  • Studies using e-beam energy dependence?
  • Mutual inductances using symmetric differences

4
Program to validate coil accuracy developed with
field-line tracing
  • Modular coils plus TF gives configuration
    sensitive to Modular coil displacements or tilts
  • Configuration is insensitive to TF misalignments.
  • The PF coils can be tested in pairs
  • The ratios of the TF, PF and MC currents are
    varied to explore different configurations.
  • Insensitive to alignment errors for PF coils 1 -
    3.
  • PF coils may also be added singly

5
Configurations sensitive to error-fields have
intrinsic islands
  • Separatrix of initial 3/6 island chain is "split"
    by 1/2 error field.
  • Modular Coil 1 shifted by 3mm.
  • Mapping near the separatrix requires many passes,
    high resolution.

V. Rudakov, Kharkov, S. Georgievski
6
Configurations with single PF coil offer
potential to isolate errors
  • PF6 lower and TF currents adjusted to give ?
    0.5 surface.
  • Intrinsic island separatrix is split, as in
    previous cases.

Peterson, et al., APS'06, Auburn CTH
45 cm
  • PF6 tilted 0.2º 10mm
  • 1mm displacement requires 1cm resolution

S. Georgievski, PPPL, V. Rudakov, Kharkov
7
Vacuum configurations will be tested with ?  0.2
to ?  0.82
iota range 0.205-0.238
  • Scans in shear will also be explored.
  • Verification of transform is goal, as well as
    shape and good surfaces.
  • Very flexible coil set gives large range of
    configurations.

iota range 0.68-0.80
iota range 0.80-1.00
S. Georgievski, PPPL, V. Rudakov, Kharkov
8
Summary
  • A plan is taking form for localizing possible
    sources of error fields to one of the three major
    coil sets (Modular coils, poloidal field coils,
    or toroidal field coils).
  • A range of vacuum configurations will be mapped
    in FY09 to validate control of field topology.
  • Auburn has offered to collaborate on field
    mapping, and to provide through loans some of the
    e-beam mapping hardware.

9
Configurations with small intrinsic islands
exist, but
10.20
  • Small increase/decrease (0.15) in vertical
    field creates large islands.
  • Questionable whether control of fields will be
    good enough to exploit this configuration.

10.06
9.84
10
The null configuration is very sensitive to
poloidal field coil tilts
  • Net tilt of 1 cm, gives 4 cm island.
  • Assuming linear scaling of error field with tilt,
    and a minimum detectable island of 1 cm
    minimum detectable tilt of PF6 is 1 mm.
  • K? 1.118, Bz(1.4)10.06.
  • PF6 tilted around X direction with angle 6.

11
"Bean" offers best access for scanning
fluorescent rods
  • Full coverage requires multiple probes.
  • But rods can be relatively short, allowing fast
    scan times.
  • Other cross-sections are being evaluated.
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