A. Adraktas Acknowledgments: V. Senaj MKD meeting, 2 April 2015 2 - - PowerPoint PPT Presentation

a adraktas
SMART_READER_LITE
LIVE PREVIEW

A. Adraktas Acknowledgments: V. Senaj MKD meeting, 2 April 2015 2 - - PowerPoint PPT Presentation

Technology MKD 3D field calculations Department MKD 3D field calculations A. Adraktas Acknowledgments: V. Senaj MKD meeting, 2 April 2015 2 April 2015 A.Adraktas 1 Technology MKD 3D field calculations Department 3D field calculations


slide-1
SLIDE 1

Technology Department

2 April 2015 A.Adraktas 1

MKD 3D field calculations MKD 3D field calculations

  • A. Adraktas

Acknowledgments: V. Senaj MKD meeting, 2 April 2015

slide-2
SLIDE 2

Technology Department

2 April 2015 A.Adraktas 2

MKD 3D field calculations

3D field calculations for the existing GTO stack

slide-3
SLIDE 3

Technology Department

2 April 2015 A.Adraktas 3

MKD 3D field calculations

3D field calculations for the existing GTO stack

slide-4
SLIDE 4

Technology Department

2 April 2015 A.Adraktas 4

MKD 3D field calculations

3D field calculations for the existing GTO stack

slide-5
SLIDE 5

Technology Department

2 April 2015 A.Adraktas 5

MKD 3D field calculations Calculation of inductance of model

Based on previously existing models in opera 2d the inductance of the gto was calculated to L≈132nH

slide-6
SLIDE 6

Technology Department

2 April 2015 A.Adraktas 6

MKD 3D field calculations Conclusions

  • According to the simulations high electric field is predicted

near the surface of the araldite around the ground busbar where the discharges have benn observed. There is also a high field near the surface of the capacitor stack. Moving the ground busbar in a larger distance from the HV conductor will probably reduce the field significantly

  • The inductance prediction is based on a previously existing
  • model. If we assume current density to be in a larger radius

than before this would give us a lower inductance of the model(ongoing)