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Abstract We have developed a portable plasma focus neutron source of 302 J energy operated by a single Maxwell capacitor (20 mF, 6 kV). The device together with the capacitor has a diameter of 10 cm, height of 37 cm and a weight of 3.78 kg. It is capable of delivering a neutron yield of the order of 10 5 neutrons per pulse with deuterium as fuel gas. For a single gas fill the device has a shelf life of 3000 shots recorded over a period of three years. Afterwards the yield is gradually deteriorated due to the deposition of sputtered kovar material on the insulator sleeve. However with a fresh gas fill the device can still serve as a source of neutrons in the lower edge of 10 4 neutrons per shot. Introduction A Mather type plasma focus machine that produces neutrons through D-D fusion reactions Energy source is a single Maxwell capacitor operated at 5.5 kV Dimensions of the system are : Height = 37 cm, Diameter = 10 cm, weight = 3.78 kg Fuel gas is deuterium Energy is transferred to the system through open air trigger Anode is in the form of a feed through composed of kovar rod brazed with Alumina insulator sleeve which is further brazed with a rotatable kovar flange The anode feed through is coupled to the vacuum chamber and cathode through a copper gaskit Results References 1. Aleksandr V. Dubrovsky, Vladymir A. Gribkov, “Installation based on high efficiency high repetition rate miniature DPF chambers for material science”, Nukleonika 2000, 45(3), PP 159-162. 2. Rishi Verma, M V Roshan, F Malik, P lee, S Lee, S V Springham, T L Tan, M Krishnan, R S Rawat, “Compact Sub-Kilojoule Range Fast Miniature Plasma Focus as Portable Neutron Source”, Plasma Sources Science and Technology, volume 17, 2008, PP1-11 3. E. J. T. Burns, S. M. Falacy, R. A. Hill, P. D. Thacher, “A high neutron output dense plasma focus”, Physics Letters A, Volume 133, Number 3, 1988, PP144-148 Development of A Low Energy Compact & Portable Plasma Focus Neutron Source Qurratul Ain, Kameel Arshad, Amjad Hussain, Abrar Ahmed Pakistan Institute of Engineering & Applied Sciences (PIEAS), Islamabad, Pakistan Main Chamber Cathode Anode Alumina Sleeve Vacuum Port 0.0 1.0 2.0 3.0 4.0 5.0 6.0 7.0 8.0 9.0 10.0 1 11 21 31 41 51 61 71 81 91 101 Neutron Yield (× 10 5 n/shot) Shot # D - D Fusion Reactions Experimental Procedure 1 D 2 + 1 D 2 = 2 He 3 + 0 n 1 3.27 MeV (Neutron Branch) 1 D 2 + 1 D 2 = 1 T 3 + 1 H 1 4.03 MeV (Proton Branch) Evacuation up to 10 -8 mb for two days Baking of assembly at 300 ˚C for 16 hours Absorption of deuterium gas in the empty sites of the chamber and electrodes. Conditioning of the system for 100 shots before regular operation Figure 2: Rogowski Coil Current Derivative Signal (Upper), and Neutron Signal from Scintillator-PMT (Lower) Figure 3: Neutron Yield Measured Vs. No of Shots With a BF 3 Detector Figure 1: Portable Plasma Focus Device (a) Complete Assembly, (b) Cross-sectional View of Plasma Tube FWHM of the neutron pulse recorded by scintillator is 38 ns A jitter of 300-400 ns is observed in the pinch pulse The pinch spike shows focus phenomenon at anode tip Plasma Tube Capacitor (a) (b) System Parameters Energy (J) Current (kA) Operating Voltage (kV) Capacitance (mF) Inductance (nH) Resistance (mΩ) Pressure (torr) FWHM (ns) Anode Radius a (mm) Cathode Radius b (mm) Anode Length (mm) Ratio b/a 302 69 5.5 20 69 40 2.5 38 7.5 20.5 90 2.7 0 1 2 3 4 5 6 0 1 2 3 4 5 6 Fill Pressure (torr) Av. Neutron Yield (× 10 5 n/shot) Figure 4: Determination of Optimum Pressure Neutron yield of the system is of the order of 10 5 neutrons per shot Shelf life of the system is 3000 shots/ gas fill for a period of more than three years. After one shelf life neutron yield is degraded by an order of magnitude The optimum pressure of the DPF system was found to be 2.5 torr Peak Average yield of 5.5 × 10 5 n/shot was observed at optimum pressure Neutron Detectors BF 3 detector (2” diameter) Plastic scintillator, NE-102 with PMT, Model-XP2020 PIEAS

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  • AbstractWe have developed a portable plasma focus neutron source of 302 J energy operated by a single Maxwell capacitor (20 mF, 6 kV). The device together with thecapacitor has a diameter of 10 cm, height of 37 cm and a weight of 3.78 kg. It is capable of delivering a neutron yield of the order of 105 neutrons per pulse withdeuterium as fuel gas. For a single gas fill the device has a shelf life of 3000 shots recorded over a period of three years. Afterwards the yield is graduallydeteriorated due to the deposition of sputtered kovar material on the insulator sleeve. However with a fresh gas fill the device can still serve as a source ofneutrons in the lower edge of 104 neutrons per shot.

    Introduction

    • A Mather type plasma focus machine that producesneutrons through D-D fusion reactions

    • Energy source is a single Maxwell capacitor operatedat 5.5 kV

    • Dimensions of the system are : Height = 37 cm,Diameter = 10 cm, weight = 3.78 kg

    • Fuel gas is deuterium• Energy is transferred to the system through open air

    trigger• Anode is in the form of a feed through composed of

    kovar rod brazed with Alumina insulator sleevewhich is further brazed with a rotatable kovar flange

    • The anode feed through is coupled to the vacuumchamber and cathode through a copper gaskit

    Results

    References1. Aleksandr V. Dubrovsky, Vladymir A. Gribkov, “Installation based on high efficiency high repetition rate miniature DPF chambers for material science”, Nukleonika 2000,

    45(3), PP 159-162.2. Rishi Verma, M V Roshan, F Malik, P lee, S Lee, S V Springham, T L Tan, M Krishnan, R S Rawat, “Compact Sub-Kilojoule Range Fast Miniature Plasma Focus as Portable

    Neutron Source”, Plasma Sources Science and Technology, volume 17, 2008, PP 1-113. E. J. T. Burns, S. M. Falacy, R. A. Hill, P. D. Thacher, “A high neutron output dense plasma focus”, Physics Letters A, Volume 133, Number 3, 1988, PP 144-148

    Development of A Low Energy Compact & Portable

    Plasma Focus Neutron Source

    Qurratul Ain, Kameel Arshad, Amjad Hussain, Abrar Ahmed

    Pakistan Institute of Engineering & Applied Sciences (PIEAS),

    Islamabad, Pakistan

    Main Chamber

    Cathode

    Anode

    AluminaSleeve

    Vacuum Port

    0.0

    1.0

    2.0

    3.0

    4.0

    5.0

    6.0

    7.0

    8.0

    9.0

    10.0

    1 11 21 31 41 51 61 71 81 91 101

    Ne

    utr

    on

    Yie

    ld (

    ×1

    05

    n/s

    ho

    t)

    Shot #

    D-D Fusion Reactions

    Experimental Procedure

    • 1D2 + 1D

    2 = 2He3 + 0n

    1 3.27 MeV (Neutron Branch)• 1D

    2 + 1D2 = 1T

    3 + 1H1 4.03 MeV (Proton Branch)

    • Evacuation up to 10-8 mb for two days• Baking of assembly at 300 ˚C for 16 hours• Absorption of deuterium gas in the empty sites of

    the chamber and electrodes.• Conditioning of the system for 100 shots before

    regular operation

    Figure 2: Rogowski Coil Current Derivative Signal (Upper), and Neutron Signal from Scintillator-PMT (Lower)

    Figure 3: Neutron Yield Measured Vs. No of Shots With a BF3 Detector

    Figure 1: Portable Plasma Focus Device (a) Complete Assembly, (b) Cross-sectional View of Plasma Tube

    • FWHM of the neutron pulse recorded byscintillator is 38 ns

    • A jitter of 300-400 ns is observed in the pinchpulse

    • The pinch spike shows focus phenomenon atanode tip

    Plasma Tube

    Capacitor

    (a) (b)

    System Parameters

    Energy (J)

    Current(kA)

    OperatingVoltage

    (kV)

    Capacitance(mF)

    Inductance(nH)

    Resistance(mΩ)

    Pressure(torr)

    FWHM(ns)

    Anode Radius

    a(mm)

    CathodeRadius

    b(mm)

    Anode Length(mm)

    Ratiob/a

    302 69 5.5 20 69 40 2.5 38 7.5 20.5 90 2.7

    0

    1

    2

    3

    4

    5

    6

    0 1 2 3 4 5 6

    Fill Pressure (torr)

    Av.

    Ne

    utr

    on

    Yie

    ld (

    ×1

    05

    n/s

    ho

    t)

    Figure 4: Determination of Optimum Pressure

    • Neutron yield of the system is of the order of105 neutrons per shot

    • Shelf life of the system is 3000 shots/ gas fill for aperiod of more than three years. After one shelf lifeneutron yield is degraded by an order of magnitude

    • The optimum pressure of the DPF system was foundto be 2.5 torr

    • Peak Average yield of 5.5 × 105 n/shot was observedat optimum pressure

    Neutron Detectors• BF3 detector (2” diameter)• Plastic scintillator, NE-102 with PMT, Model-XP2020

    PIEAS