ssx summary: helicity balance and ohms law

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Workshop on Magnetic Self-Organization NSF Center meeting, Aug 4-6, 2004 Michael Brown C. D. Cothran, J. Fung, A. O Murchadha, Z. Michielli, M. Chang Swarthmore College Collaborators: M. Schaffer (GA), W. Matthaeus (Bartol), D. Cohen (Swarthmore), E. Belova (PPPL) Research supported by US DOE grants ER54604 and ER54490 SSX summary: helicity balance and Ohms law

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SSX summary: helicity balance and Ohms law. Workshop on Magnetic Self-Organization NSF Center meeting, Aug 4-6, 2004 Michael Brown C. D. Cothran, J. Fung, A. O Murchadha, Z. Michielli, M. Chang Swarthmore College Collaborators: M. Schaffer (GA), W. Matthaeus (Bartol), - PowerPoint PPT Presentation

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Page 1: SSX summary: helicity balance and Ohms law

Workshop on Magnetic Self-OrganizationNSF Center meeting, Aug 4-6, 2004

Michael BrownC. D. Cothran, J. Fung, A. O Murchadha, Z. Michielli, M. Chang

Swarthmore College

Collaborators: M. Schaffer (GA), W. Matthaeus (Bartol),D. Cohen (Swarthmore), E. Belova (PPPL)

Research supported by US DOE grants ER54604 and ER54490

SSX summary: helicity balance and Ohms law

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Outline

A brief tour of the Swarthmore Spheromak Experiment (SSX)Device, diagnostics, plasma parameters

Full merging and self-organization to large scale(magnetic helicity conservation, FRC, doublet CT)

Local 3D magnetic reconnection studies(generalized Ohms law, Hall terms, energetic ions)

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Full merging: FRC formation

Right-handedSpheromak

Left-handedspheromak Large scale structure (FRC)

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Magnetic structure consistent with FRC/doublet-CT

full data

•m=0 dominates•Other modes are present

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Magnetic reconnection in three dimensions

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Reconnection in SSX-FRC

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Ensemble average of 36 identical shots

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PART 1

Helicity balance

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Spheromak formation

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Complete merging: FRC formation

Right-handedSpheromak

Left-handedspheromak

FRC

Helicity conservation leads to a null helicity structure

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The SSX Laboratory

10kV/100kAPulsed power

Cylindrical flux conservers andvacuum chamber (=0.40m, L=0.65m)

Coaxial magnetized plasmaguns on each end (1 mWb)

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Diagnostics at SSX

600 channel 1.25 MHz data acquisition system

Magnetic probe arrays

Langmuir triple probe

He-Ne quadrature interferometer

0.2 m VUV monochrometer

Bolometer

Retarding Grid Energy Analyzers (RGEA)

Soft x-ray photodiodes (SXR)

Directional (Gundestrup) Mach probe

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Distributed probe array

12 probe stalks: 4 toroidally at three axial positions

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Magnetic structure consistent with FRC/doublet-CT

m=0 (toroidal mode) component

•Reversed field•Very little midplane toroidal field•Axially antisymmetric B•70 G RCC field (on axis)

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Magnetic structure consistent with FRC/doublet-CT

full data

•m=0 dominates•Other modes are present

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Peak poloidal flux and radial flux profile

•Ends reach 3-4 mWb immediately (3-4 amplification)•Midplane flux grows to match ends•Reconnection rate ≈ 0.04•No private flux after 50s, but toroidal fields remain•Midplane flux profile consistent with RS/√2: high FRC

70 G RCC field (on axis)

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Axisymmetric helicity estimate

• Poloidal flux = 3 mWb (east and west)

• Toroidal flux = +/- 3 mWb (east and west)

• Helicity = 2x10 mWb^2 east – 2x10 mWb^2 west = zero total

• Rate = 2(1 kV)(1 mWb) x 10 s = 20 mWb^2

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m=1 component late in time: tilted CT

Geometric axis of CT is perpendicular to the flux conserver axis

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Elena Belova 2D simulation

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3D simulation showing tilt instability

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Full data (70 G on axis)

QuickTime™ and aTIFF decompressor

are needed to see this picture.

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PART 2

Generalized Ohm’s Lawand Energetic Ions

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3D magnetic reconnection experiments

Brown et al Astrophys. J. Lett. (9/02)Brown et al Phys. Plasmas 9, 2077 (2002)Brown et al Phys. Plasmas 6, 1717 (1999)Kornack et al Phys. Rev. E 58, R36 (1998)

Magnetic probe array

RGEAs

Large slots cut into FC rear walls define the reconnection region

3D magnetic propertiesEnergetic particles

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3D magnetic probe array

600 coils, 558 array

~2 cm spacing

25 three channel 8:1multiplexer/integratorboards

10 eight channel 8-bitCAMAC digitizers

Full probe readoutevery 0.8 s

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Reconnection in SSX-FRC

Catch reconnection early (< 32 s) then FRC forms

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Generalized Ohms Law and Curl

• E + vxB = ηJ + (JxB – grad P)/ne + ∂J/∂t

• Curl (vxB + div P) =

∂B/∂t + Curl ηJ + Curl (JxB)/ne + Curl (∂J/∂t)

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Hall term dominates electric field during shot

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Ensemble average of 36 identical shots

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Terms in curl of Ohms law (single shot)

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Generalized Ohm’s Law magnitudes

• E + vxB = ηJ + (JxB – grad P)/ne + ∂J/∂t

• Ohmic and electron inertia terms are small

• From near pressure balance and unity , we know that JxB and grad P are comparable

• Only grad P can contribute at the neutral line

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In plane magnetic field (ala min variance)

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Out of plane magnetic field

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Merger of left and right handed tori

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Side view

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Cross section

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In plane JxB force (ala min variance)

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Out of plane JxB force (slingshot)

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Current channel formation correlates with RGEA activity

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RGEA raw signals

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Average peak signal for the out-of-plane RGEA

Fit to a thermal distribution with drift:T=33±11eV and V=86±20eV

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SummarySpheromak merging in SSX forms large scale,

self-organized structure•Reconnection is fully 3D

•Merging results in self-organized structure •Helicity conservation implies null helicity

•Hall terms dominate electric field in Ohms law

•Study dynamics of doublet-FRC •Study flow with Mach probe, ion doppler•Need computational/theoretical support

Local SSX reconnection is fully 3D, generates energetic particles, flow, and heat

Page 42: SSX summary: helicity balance and Ohms law

Plans for the near future

• Implement IDS at midplane of SSX-FRC (use with Mach probe)

• Compare flow results with Belova code

• Helium glow discharge cleaning for density control (lower density, larger c/pi)