Difference between revisions of "HEDP notes"
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*14 MBar at 140 kA at 15-um radius (shot 634 with 2x30-um W wires) | *14 MBar at 140 kA at 15-um radius (shot 634 with 2x30-um W wires) | ||
*25 MBar at 150 kA at 12-um radius (shot 657 with 2x30-um Mo wires) | *25 MBar at 150 kA at 12-um radius (shot 657 with 2x30-um Mo wires) | ||
− | * | + | *100 MBar at 154 kA at 6-um radius (shot 657 with 2x30-um Mo wires) |
=Links= | =Links= | ||
*[http://www.nap.edu/read/10544/chapter/1 Frontiers in High Energy Density Physics THE X-GAMES OF CONTEMPORARY SCIENCE] | *[http://www.nap.edu/read/10544/chapter/1 Frontiers in High Energy Density Physics THE X-GAMES OF CONTEMPORARY SCIENCE] |
Revision as of 02:53, 1 April 2016
high energy density plasma is a plasma with pressure above 1 MBar
magnetic field produced by single wire (Biot-Savart Law)
- 10 MA at 4 mm radius is 500 T
- 100 kA at 40 um radius is 500 T
- 160 kA at 5 um radius is 6,400 T
magnetic pressure
- 10 MA at 4 mm radius is 1 MBar
- 100 kA at 40 um radius is 1 MBar
- 160 kA at 5 um radius is 164 MBar
Bennett condition
- magnetic pressure = plasmakinetic pressure
- 100 kA at 40-um radius is 1 MBar of plasma pressure
- 100 kA at 1-um radius is 1.6 GBar of plasma pressure
@-LTD-Bricks x-pinches
- 14 MBar at 140 kA at 15-um radius (shot 634 with 2x30-um W wires)
- 25 MBar at 150 kA at 12-um radius (shot 657 with 2x30-um Mo wires)
- 100 MBar at 154 kA at 6-um radius (shot 657 with 2x30-um Mo wires)