Abstract:The dynamics of the dense plasma near the cross point of an X pinch has been investigated using 1 ns x-ray backlighting images at different moments relative to the start of 100 ns [full width at half maximum (FWHM)] 200 kA current pulses. If the two metal wires are fine enough (e.g., 10 μm W or 17.5 μm Mo) to form a pinch at the cross point, accompanied by an x-ray burst, with the available current pulse, then the images show three stages of development: a radial explosion/expansion phase; an implosion during … Show more
“…8,9 These hot spots are of great interest for their high energy density conditions and are used as a source for high energy radiography. 7,[10][11][12][13][14][15] Following the x-ray burst, plasma is rapidly evacuated from the central region, leaving a gap in the axial density profile which continually expands late in time. 7,13,16 Much of the research on x-pinches has been to characterize the implosion dynamics at the cross point, in order to more fully understand the x-ray generation mechanics.…”
Section: Introductionmentioning
confidence: 99%
“…7,[10][11][12][13][14][15] Following the x-ray burst, plasma is rapidly evacuated from the central region, leaving a gap in the axial density profile which continually expands late in time. 7,13,16 Much of the research on x-pinches has been to characterize the implosion dynamics at the cross point, in order to more fully understand the x-ray generation mechanics. 7,13 A substantial amount of work on the examination of x-pinch dynamics has been carried out with the use of x-ray backlighters, using x-pinches in parallel load configurations ͑us-ing the x-ray burst from one to image the other͒.…”
Section: Introductionmentioning
confidence: 99%
“…[4][5][6] At the same time, the self-generated magnetic field from the flow of current combines at the cross point to create a strong global field that compresses the plasma to near solid densities, forming a z-pinch that is a few hundreds of micrometers in length, often referred to as a micro z-pinch. 7 Magnetohydrodynamic instabilities lead to pinching of the plasma at multiple points along the micro z-pinch. Some of these pinching points develop into "hot spots" of high density and temperature plasma that emit intense bursts of soft x-ray radiation, in the 1 -10 keV range, that can have subnanosecond duration.…”
Section: Introductionmentioning
confidence: 99%
“…7,13,16 Much of the research on x-pinches has been to characterize the implosion dynamics at the cross point, in order to more fully understand the x-ray generation mechanics. 7,13 A substantial amount of work on the examination of x-pinch dynamics has been carried out with the use of x-ray backlighters, using x-pinches in parallel load configurations ͑us-ing the x-ray burst from one to image the other͒. 7,13,[17][18][19] Radiography has also been used in conjunction with selfemission soft x-ray imaging to examine differences in the dynamics and output of two-and four-wire x-pinch configurations.…”
Studies of the late time diode gap formation in two- and four-wire tungsten x-pinches using an 80kA, 50ns current pulse are presented. Quantitative measurements of the coronal plasma density are recovered using interferometry simultaneously with laser shadowgraphy. Axial expansion of the gap occurs at ∼106cm∕s for both two- and four-wire systems and is likely to be driven by an axial J×B force resulting from radial current flow in the plasma minidiode “electrodes.” Radial density profiles suggest repinching of the low density plasma occurs after the main pinch resulting in secondary x-ray emission peak >10ns after the first, which is recorded with a pair of pin diodes.
“…8,9 These hot spots are of great interest for their high energy density conditions and are used as a source for high energy radiography. 7,[10][11][12][13][14][15] Following the x-ray burst, plasma is rapidly evacuated from the central region, leaving a gap in the axial density profile which continually expands late in time. 7,13,16 Much of the research on x-pinches has been to characterize the implosion dynamics at the cross point, in order to more fully understand the x-ray generation mechanics.…”
Section: Introductionmentioning
confidence: 99%
“…7,[10][11][12][13][14][15] Following the x-ray burst, plasma is rapidly evacuated from the central region, leaving a gap in the axial density profile which continually expands late in time. 7,13,16 Much of the research on x-pinches has been to characterize the implosion dynamics at the cross point, in order to more fully understand the x-ray generation mechanics. 7,13 A substantial amount of work on the examination of x-pinch dynamics has been carried out with the use of x-ray backlighters, using x-pinches in parallel load configurations ͑us-ing the x-ray burst from one to image the other͒.…”
Section: Introductionmentioning
confidence: 99%
“…[4][5][6] At the same time, the self-generated magnetic field from the flow of current combines at the cross point to create a strong global field that compresses the plasma to near solid densities, forming a z-pinch that is a few hundreds of micrometers in length, often referred to as a micro z-pinch. 7 Magnetohydrodynamic instabilities lead to pinching of the plasma at multiple points along the micro z-pinch. Some of these pinching points develop into "hot spots" of high density and temperature plasma that emit intense bursts of soft x-ray radiation, in the 1 -10 keV range, that can have subnanosecond duration.…”
Section: Introductionmentioning
confidence: 99%
“…7,13,16 Much of the research on x-pinches has been to characterize the implosion dynamics at the cross point, in order to more fully understand the x-ray generation mechanics. 7,13 A substantial amount of work on the examination of x-pinch dynamics has been carried out with the use of x-ray backlighters, using x-pinches in parallel load configurations ͑us-ing the x-ray burst from one to image the other͒. 7,13,[17][18][19] Radiography has also been used in conjunction with selfemission soft x-ray imaging to examine differences in the dynamics and output of two-and four-wire x-pinch configurations.…”
Studies of the late time diode gap formation in two- and four-wire tungsten x-pinches using an 80kA, 50ns current pulse are presented. Quantitative measurements of the coronal plasma density are recovered using interferometry simultaneously with laser shadowgraphy. Axial expansion of the gap occurs at ∼106cm∕s for both two- and four-wire systems and is likely to be driven by an axial J×B force resulting from radial current flow in the plasma minidiode “electrodes.” Radial density profiles suggest repinching of the low density plasma occurs after the main pinch resulting in secondary x-ray emission peak >10ns after the first, which is recorded with a pair of pin diodes.
“…Plasma focus (PF) is among the low-priced available neutron and ions generators, with unique features of extremely short pulses (hundreds of ns) that suit it for different interesting applications [3][4][5][6]. Similarly, the soft X-rays emitted from PF have attracted the many researchers due to large numbers of application such as high brightness source for lithography in order to fabricate the electronic devices, X-ray laser pumping, X-ray Microscopy, X-ray backlighting and radiography [7][8][9][10][11][12].…”
The effect of pre-ionization caused by depleted uranium ( 92 U 238 ) on the correlation of neutron and X-ray emission from 1.8 kJ plasma focus is investigated by employing photomultiplier tubes (XP2020) coupled with fast (50 9 50) mm 2 cylindrical plastic scintillators (NE102A) along with GM tube and Quantrad Si PIN diodes with a pair of appropriate filters. It is found that neutron and Cu-K a emission along with total X-ray yield are significantly increases with pre-ionization as compared to those without pre-ionization. Moreover, pre-ionization improves the shot to shot reproducibility of the system and broadens the operating pressure regime both for neutron and X-ray emission.
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