FXR discharges at various pressures

Englund, Ann-Kristin; Händel, S. K.

doi:10.1007/bf01394685

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1970

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“…Calculation of U. Inserting Eqs. (7), (9), and ( 10) in (l), we obtain m a=- in Eq. (ll), one obtains for the "feeding velocity" u = 2 x IOB cmjsec.…”

Section: W =mentioning

confidence: 77%

“…The energy Q is then expressed by the equation (9) In the calculation of Q the radiation losses have been neglected. Estimation of T. Temperatures of the order of 30 00040 000 K have been measured in the Garton flash tube [13-141. As the FXR tube used here is of similar construction to that by Garton (low inductance) it can be assumed that the temperature in the present case is of the order of 30000 K even though the input energy is slightly lower here.…”

Section: W =mentioning

confidence: 99%

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Anode Vapour Flow Phenomena in a FXR Discharge

1970

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Streak photographs of the radial motion of vaporized electrode material in a flash X-ray (FXR) discharge indicate successive constrictions of the metal vapour cloud existing just outside the anode. Such a constriction may give rise to the anode vapour jet earlier observed in axial streak photographs of the discharge. Calculations show that the anode vapour production is sufficiently high to supply the discharge column behind the jet front with "new" vapour.

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“…Calculation of U. Inserting Eqs. (7), (9), and ( 10) in (l), we obtain m a=- in Eq. (ll), one obtains for the "feeding velocity" u = 2 x IOB cmjsec.…”

Section: W =mentioning

confidence: 77%

Section: W =mentioning

confidence: 99%