Difference between revisions of "HEDP notes"

From New IAC Wiki
Jump to navigation Jump to search
Line 32: Line 32:
 
*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)
*25 MBar at 154 kA at 6-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

go back

high energy density plasma is a plasma with pressure above 1 MBar

[math]1 MBar = 1 \times 10^6 \times 10^5 Pa = 10^{11} Pa = 10^{11} (N m)/(m^2) = 10^{11} J/m = 10^{11} (10^7 erg)/(10^6 cm^3) = 10^{12} erg/cm^3[/math]


magnetic field produced by single wire (Biot-Savart Law)

[math]B[G] = 0.2 \times I(A) / r(cm) [/math]
[math]B[T] = 0.2 \times I(kA) / r(mm) [/math]
  • 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

[math] P_m(bar) = 4 \times B(T)^2 [/math]
[math] P_m(bar) = 0.16 \times I(kA)^2 \times R(mm)^{-2} [/math] 
  • 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)

Links