1 / 21

U. Konopka

Max-Planck-Institute for Extraterrestrial Physics. New, „Flexible“ Plasma Devices for Complex Plasma Experiments. U. Konopka. Max-Planck-Institut für Extraterrestrische Physik, Giessenbachstrasse, 85741 Garching, Germany. email : konopka@mpe.mpg.de. Why do we design new plasma chambers for

naasir
Télécharger la présentation

U. Konopka

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Max-Planck-Institute for Extraterrestrial Physics New, „Flexible“ Plasma Devices for Complex Plasma Experiments U. Konopka Max-Planck-Institut für Extraterrestrische Physik, Giessenbachstrasse, 85741 Garching, Germany email: konopka@mpe.mpg.de

  2. Why do we design new plasma chambers for complex plasma experiments ? With the new setups we would like to reach experimental conditions that go far beyond what can be established with former designs as i.e.: PKE-Nefedov: Single parallel plate discharge PK3-Plus: Single parallel plate discharge (much more flexible and quality optimized) PK4: DC-Discharge tube (addresses different complex plasmas physics (i.e. flows)) IMPF-Predevelopment chambers: Cylindrical Chamber (capacitive) Spherical Chamber (inductive) Spherical Chamber (capacitive)

  3. Experiences from the IMPF (Pre-)Developments Spherical Chamber (inductive) Spherical Chamber (capacitive) B RF-1

  4. Experiences from the IMPF (Pre-)Developments Spherical Chamber (inductive) Spherical Chamber (capacitive) RF-2 RF-3 Random switched RF parallel plate discharge RF-1

  5. Experiences from the IMPF (Pre-)Developments Spherical Chamber (inductive) Spherical Chamber (capacitive)

  6. Labor experiences using the IMPF RF chamber Experimental setup

  7. Labor experiences using the IMPF RF chamber A Transparent Top Electrode A transparent (ITO-covered) conducting (RF) top electrode was introduced. camera a single particle camera New single electrode (Ø ≈ 80mm, groove Ø ≈ 40 mm, 1 mm depth) used for potential measurements, single particle manipulation

  8. y x Labor experiences using the IMPF RF chamber The Electrode System α Fc(x)= mg·sin(α) mg

  9. Goals for removing former constrains and their implications? Limited plasma parameter range: Limited system geometries: Void, Ellipsoids Adaptive, Multi-Clouds Limited manipulation devices: Function generator Adaptive Elec., Laser Twizers,.. Limited interaction variation: Debye-Hückel Designer-Potential (attractive)

  10. Two new design approaches will be studied Zyflex - Chamber Zyflex - Chamber Dodecahedron - Chamber Flexible plasma chamber with quasi spherical geometry and timeaveraged isotropic plasma structure Flexible, parallel plate discharge chamber with improved electrode setups

  11. The Zyflex-Chamber - Concept Variable shower head/electrode holder combination Modular parallel plate electrode system

  12. The Zyflex-Chamber – Gasflow and Plasmastructure for pumping and dust removal

  13. The Zyflex-Chamber – Elektrode modules Single RF-Electrode (maybe transparent) Double RF-Electrode (maybe transparent) Adaptive RF-Electrode Double DC-RF Combi Electrode Adaptive DC-RF Combi Electrode (maybe with second grid for active electron temperature control)

  14. The Zyflex-Chamber - Implications Extended plasma parameter range (√) Extended system geometries√ Extended manipulation devices√ Extended interaction variation (√)

  15. Two new design approaches will be studied Zyflex - Chamber Dodecahedron - Chamber Zyflex - Chamber Flexible plasma chamber with quasi spherical geometry and timeaveraged isotropic plasma structure Flexible, parallel plate discharge chamber with improved electrode setups

  16. The Dodecahedron-Chamber – Background The attractive potential Ion flow and ion-wake-potential in 2D In the limit of smooth angular Variation of the ion flow the timeaveraged potential will be quasi spherical. With increasing pressure the crytical angle for a smooth potential is increasing. With a smooth controllable ion flow direction, even dedicated non spherical Potentials might be established. – Disadvantage: Orientation is globally fixed.

  17. RF DC The Dodecahedron-Chamber - Concept The plasma generation (Example 2D) The real chamber should be driven by 12 independend rf-generators that can be individually shifted in phase, have different, programmable output power as well as an arbitrary DC-offset – everthing software controlled (>10kHz).

  18. The Dodecahedron-Chamber - Concept The plasma generation RF DC Timeaveraged quasi isotropic plasma in 2D/3D – Dodecahedron geometry But, why a dodecahedron?

  19. The Dodecahedron-Chamber - Concept The plasma generation RF DC Time averaged By continuous dc-voltage control the Ion-drag should be smoothed directionable 3D

  20. The Dodecahedron-Chamber Extended plasma parameter range√! Extended system geometries (√) Extended manipulation devices√ Extended interaction variation√!

  21. The Dodecahedron-Chamber Thank‘s for your attention.

More Related