HEDP notes: Difference between revisions
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[https://wiki.iac.isu.edu/index.php/RS#Pulsed-power_applications_.282-LTD-driver_and_more.29 go back] | [https://wiki.iac.isu.edu/index.php/RS#Pulsed-power_applications_.282-LTD-driver_and_more.29 go back] | ||
=high energy density plasma | =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> | <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 ( | =magnetic field produced by single wire (Biot-Savart Law)= | ||
<math>B[ | <math>B[T] = \mu I / ( 2\pi r ) </math> | ||
*10 MA at 4 mm radius is 500 T | *10 MA at 4 mm radius is 500 T | ||
*100 kA at | *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 | |||
*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= | ||
* | *[http://www.nap.edu/read/10544/chapter/1 Frontiers in High Energy Density Physics THE X-GAMES OF CONTEMPORARY SCIENCE] | ||
Latest revision as of 18:13, 31 May 2017
high energy density plasma is a plasma with pressure above 1 MBar
[math]\displaystyle{ 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]\displaystyle{ B[T] = \mu I / ( 2\pi r ) }[/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]\displaystyle{ P_m(bar) = 4 \times B(T)^2 }[/math] [math]\displaystyle{ 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
- 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)