Bin-Xiong Yu’s research while affiliated with Spine Institute Northwest and other places

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Publications (12)


(a) The experimental cavity. (b) The equivalent circuit diagram of the measurement method. The electrodes can be equivalent to a capacitor C1 and a variable resistor R1. U0 is the high voltage supply; U1 is the input voltage; U2 is the output voltage; I is the emission current; C2 is the input capacitor; C3 is the output capacitor; R2 is the input resistor; R3 is the output resistor; L1 is the input inductor.
Characteristics of emission currents under different electric fields: (a) 304 SS, (b) Cu, and (c) Ti. The first line of the pictures is the waveforms of electric field strength and emission current under VW I. The second line is the waveforms under VW II. The third line is the waveforms under VW III.
The regulation of the emission starting points and the emission currents of 304 SS under VW III: (a) E-t and (b) ∂²E/∂t²-t. The electric field strength is 400 and 750 kV/cm.
Comparison of average emission currents of (a) 304 SS, (b) Cu, and (c) Ti under voltage I, voltage II, and voltage III. The Cu electrodes get breakdown when the electric field strength rises to 600 kV/cm. The FE threshold of Ti electrodes is 550 kV/cm.
The average current durations of (a) 304 SS, (b) Cu, and (c) Ti electrode.

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The field emission characteristics under transient electric field
  • Article
  • Publisher preview available

December 2024

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56 Reads

Yue Wu

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Jian-cang Su

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Jia-ru Shi

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[...]

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Bin-xiong Yu

This article concentrates on the field emission (FE) characteristics under the pulsed transient electric field. Experimental measurements are carried out by applying direct current (DC) voltage, millisecond pulse voltage, and microsecond pulse voltage. Additionally, 304 stainless steel, oxygen-free copper and titanium electrodes are utilized to verify the consistency. Compared with the case under DC electric field, three distinctive FE characteristics are observed under pulsed transient electric field: the regular emission, the intense emission, and the annihilation phenomenon. First, the emission starting point implies one strong correlation with the second partial derivative of transient electric field strength with respect to time. Second, the emission current under pulsed electric field is much higher than that under the DC electric field. Moreover, the FE current is deeply associated with the gradient of the electric field during the rising front. Third, the FE current is extinguished though there is still high transient electric field. The mechanism of the three characteristics is still unclear and should be the subject of further investigation.

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Method of Measuring Field Emission Current Under High-Voltage Pulse

July 2024

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25 Reads

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1 Citation

IEEE Transactions on Plasma Science

A method of measuring field emission current under high-voltage (HV) pulse is proposed. The method makes it more convenient to study electron emission under HV pulse. Based on the Kirchhoff law, this method can fundamentally solve the problem, which the emission current is usually covered up by the displacement current. In addition, the method can ensure the safety of oscilloscope and the accuracy of the measurement when the gap gets breakdown. The resolution analysis of this method is carried out. The resolution is positively correlated with the output resistance and negatively correlated with the summation of output capacitance and electrodes capacitance. The resolution, under microsecond and millisecond HV pulse, can achieve μ\mu A to A class. The measurement platform based on this method contains an energy-storage capacitor, a load resistor, an HV pulse power supply, an electrode cavity, and three resistor–capacitor ( R – C ) voltage dividers.


A Novel Screw-Based Probe to Measure Pulse Forming Line Voltage in Tesla-Type Generators

December 2019

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84 Reads

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3 Citations

IEEE Transactions on Plasma Science

A novel screw-based probe is put forward to measure the pulse forming line (PFL) voltage in Tesla-type generators. This probe utilizes an existing screw as the key part of the conventional probe. Therefore, no extra hole is needed, which simplifies the design of the PFL. The voltage ratio of this probe is not a constant which varies within the pulsewidth with a deviation of ±5%. By analysis, it is found that this deviation is mainly due to the complicated electromagnetic environment on the outer magnetic core of the Tesla transformer where this probe is assembled. The electromagnetic environment can cause perturbation which adds on the main test waveform when the Tesla transformer is charging. Two solutions are proposed for this question. One is to consider the voltage ratio as a time-dependent variable, rather than a constant any more. The other is to redesign the screw-based probe and assemble it where the electromagnetic environment is weak. Both the methods can decrease the deviation of the voltage ratio to a level smaller than 1% and are applied in practical measurements.



De-Excitation of Excited States in a Nitrogen Switch After Discharge

February 2019

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8 Reads

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1 Citation

IEEE Transactions on Plasma Science

The de-excitation of nitrogen excited states after spark gap discharge was investigated with time-resolved optical emission spectroscopy method. Recombination of ionized particles was experimentally proved less than several tens microseconds. After the recombination process, it was shown that atomic nitrogen in ground state [N( 4 S)] and molecular nitrogen in first excited state [N 2 (A 3 Σ + u )] was long-lived particles (metastable state) after gas discharge. Characteristics of decay for N(4S) and [N 2 (A 3 Σ + u )] were studied, and their lifetime and decay of density were estimated in this paper. Peculiar unexponential decay of N 2 (A 3 Σ + u ) showed there was reproduction process of N 2 (A 3 Σ + u ) after gas discharge. N(4S) could be the source for reproduction process under their mechanism of three-body recombination. Low ionization energy and high ionization collision cross section of N2(A3Σ+u ) make it a possible factor limiting the switch recovery. The de-excitation of metastable states opens novel perspectives for understanding the recovery of gas switch.


An Improved Match Method of Capacitive Divider for Measurement of Nanosecond-Range HV Pulses

December 2018

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131 Reads

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7 Citations

IEEE Transactions on Instrumentation and Measurement

In this paper, a new match circuit of the capacitive divider is studied. Using the proposed match circuit, the signal measured by the capacitive divider will not be secondarily attenuated near the accelerator, and the secondary attenuation is done at the terminal end of the cable which is located in a shielding room with a good electromagnetic environment. So, the proposed circuit has a better anti-interference capability than the traditional terminal-end match circuit. The result of the theoretic analysis shows that the proposed match circuit is equivalent with the traditional terminal-end match circuit when the parameters of the circuit are well chosen. Rectangular pulse response of the proposed match circuit is tested based on an equivalent circuit. It shows that the proposed match circuit has a good pulse response characteristic for rectangular pulse with a rise time of 5 ns, and the output waveform of the match circuit has a flattop jitter less than 1%. The match circuit proposed in this paper is utilized to measure the diode voltage of the accelerator in our laboratory. It is found that the high-frequency interference on the output waveform measured by the new match circuit is much smaller than that measured by the traditional terminal-end match circuit, which proves that the match circuit proposed in this paper is an effective method for increasing the signal-to-noise ratio of capacitive divider for measurement of nanosecond-range HV pulse.



A quasi-coaxial HV rolled pulse forming line

September 2018

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43 Reads

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8 Citations

A quasi-coaxial high-voltage (HV) rolled pulse forming line (rolled PFL) is researched in this paper. The PFL is rolled n circles on a support cylinder simultaneously by two layers of copper foil electrodes and two layers of insulation dielectrics. The first circle of the two electrodes are elicited in opposite directions along the axis, acting as the quasi-coaxial output structure of the PFL, and the left n − 1 circles of the PFL form a complete rolled strip line of n − 1 circles. The rolled PFL is convenient to realize HV insulation and is able to output a pulse with good quality. Characteristic parameters of the PFL are designed theoretically. Besides, the pulse discharge process of the PFL is simulated by computer simulation technology (CST) modeling, and the simulation result verifies the correctness of theory design. Furthermore, a rolled PFL with a characteristic impedance of 4.4 Ω is developed. The test characteristic impedance of the developed PFL by the incident pulse method confirms to the theory design. The discharge voltage waveform with a full width at half maximum of 57 ns of the PFL is acquired, which has a rise time of 6.8 ns. The HV test of the rolled PFL is carried out, and a discharge current pulse with an amplitude of 7 kA is acquired when the PFL is charged to 70 kV. It is calculated that the developed PFL has an energy storage density of 2.5 J/l. A Tesla generator based on 13 stages of rolled PFLs is designed, which is expected to output a 450 kV pulse with a duration of 100 ns on a 40-Ω match load. The discharge waveform of the generator is simulated by the CST software. The simulative output pulse has a rise time of 5 ns, with a flattop jitter less than 5%.


Fig. 3. Normalized magnetic flux density versus R/d in insulation dielectric of the RSL: (a) w 0 = π; (b) w 0 = 0.03π.
Fig. 4. A simplified sketch map of the coaxial-output RSPFL consisting of an RSL and a COE.
Fig. 5. Stretch of the COE:1, inner electrode; 2, insulation support; 3, outer electrode; 4, cover of the cavity; 5, connective electrode; 6, rectangular hole; 7, perforating strip hole.
Parameters of the RSPFL in the CST modeling compared with the design value
A coaxial-output rolled strip pulse forming line based on multi-layer films

January 2018

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176 Reads

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12 Citations

Laser and Particle Beams

A coaxial-output rolled strip pulse-forming line (RSPFL) with a dry structure is researched for the purpose of miniaturization and all-solid state of pulse-forming lines (PFL). The coaxial-output RSPFL consists of a coaxial-output electrode (COE) and a rolled strip line (RSL). The COE is characterized by quasi-coaxial structure, making the output pulse propagate along the axial direction with a small output inductance. The RSL is rolled on the COE, whose transmission characteristics are analyzed theoretically. It shows that the RSL can be regarded as a planar strip line when the rolling radius of the strip line is larger than 60 times of the thickness of the insulation dielectric layer of RSL. CST modeling was carried out to simulate the discharging characteristic of the coaxial-output RSPFL. It shows that the coaxial-output RSPFL can deliver a discharging pulse with a rise time <6 ns when the impedance of the RSL matches that of the COE, which confirms the theoretical analysis. A prototype of the coaxial-output RSPFL was developed. A 49-kV discharging pulse on a matched load was achieved when it was charged to 100 kV. The discharging waveform has a pulse width of 32 ns, with a rise time of 6 ns, which is consistent with the simulation waveform. An energy-storage density of 1.9 J/L was realized in the coaxial-output RSPFL. By the method of multi-stage connection in series, a much higher output voltage is convenient to be obtained.


Analysis on match problem of capacitive voltage divider with long measurement cable

August 2017

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254 Reads

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5 Citations

Research is carried out on the basis of the traditional two-end matched circuit of a capacitive voltage divider with a long measurement cable. Transmission progress in the circuit is analyzed theoretically. A match condition of the circuit is acquired, which requires that the circuit satisfies two conditions: (1) the measurement error should be small for a pulse with a duration of less than twice the delay time of the measurement cable; (2) the initial division ratio and the stable division ratio of the circuit are the same. Two matched methods of the circuit are acquired, including the first-order matched method and the second-order matched method. Numerical simulations are carried out. According to the simulation results, the relative errors of the circuits with a cable of 20 m are less than 1.5%, obtained by using both match methods for measurement of rectangular pulses with rise and fall times of 5 ns. An improved circuit is presented, which is suitable for any situation where the low-voltage capacitance of the capacitive divider is even smaller than the capaictance of the measurement cable. A verification experment is carried out, and the test result confirms the simulation result.


Citations (10)


... The experimental platform can measure the FE currents under both DC electric field and pulsed transient electric field. 24 According to the Kirchhoff's law, at the red point K The equivalent circuit diagram of the measurement method. The electrodes can be equivalent to a capacitor C 1 and a variable resistor R 1 . ...

Reference:

The field emission characteristics under transient electric field
Method of Measuring Field Emission Current Under High-Voltage Pulse
  • Citing Article
  • July 2024

IEEE Transactions on Plasma Science

... The High voltage generation recently become more important due to their applications such that medical applications, and testing devices [1,2]. Marx generator [3,4], Van de Graff [5,6], and Tesla Coil [7,8] are examples of high voltage generators. Tesla transformers are superior compared to other two high voltage generators. ...

A Novel Screw-Based Probe to Measure Pulse Forming Line Voltage in Tesla-Type Generators

IEEE Transactions on Plasma Science

... 10 A theory has also been provided for the matching conditions between the multistage annular PFL and the coaxial PFL. 11,12 Based on this research, this study develops and tests a mixed PFL to significantly improve the quality of the waveform of the output pulse in this type of generator. A 5-GW Tesla-type pulse generator based on the mixed PFL is proposed, and experiments are reported to verify its technical feasibility. ...

Two Methods on Pulse Shaping for a Series Coaxial Multilayered Film-Winded Pulse-Forming Line

IEEE Transactions on Plasma Science

... The breakdown voltage for the gas switch and the output voltage on load are measured by the capacitive divider installed on the PFL and TL, respectively. The accuracy is within 1% for these two capacitive dividers [18]. The conducting current on load is measured by a double-winding Rogowski coil made of two radial half-cycle coils in parallel. ...

An Improved Match Method of Capacitive Divider for Measurement of Nanosecond-Range HV Pulses

IEEE Transactions on Instrumentation and Measurement

... 14, 15 The other perspective argues that anode atoms are evaporated as the anode being heated to high temperature. [16][17][18][19] Experimental measurements by Grissom and Newton 20 and Boxman 21 revealed that anode surface temperature could exceed its melting point, but the reported anode temperatures varied from several thousand kelvins across different experiments, and the primary source of anode heating remained unconfirmed. 21,22 Inada et al. 17 and Nagai et al. 19 suggested that electron bombardment heating anode to generate anode plasma based on the phenomenon of anodic flare appearing before cathodic flare. ...

Investigation of vacuum gap breakdown under microsecond pulses

IEEE Transactions on Dielectrics and Electrical Insulation

... The transfer function of an ideal CVD is independent of frequency. However, the actual transfer function of the CVD may be influenced by the loading effect of the measuring cables and low-voltage measurement equipment [77,79] as illustrated in Figure 8. ...

Analysis on match problem of capacitive voltage divider with long measurement cable

... For the formula for vacuum breakdown in (36) and (37), the effect of time holds from 1 ns to 10 μs, as reported in [13, p. 420], and is replotted in Fig. 8. The range for the effect of the vacuum gap on E v ranges from 0.4 to 400 cm [13] and that for the effect of area on E v ranges from 2 × 10 3 to 7 × 10 5 cm 2 [17]. ...

A Method to design composite insulation structures based on reliability for pulsed power systems

Laser and Particle Beams

... The total length of the tape is therefore being expressed as Equation (7) [27,28]. The formula can be used to determine the parameter of vertical turn; vertical length and number of turn required for primary and secondary coils. ...

Parametric calculation of pulse transformer with open magnetic cores based on magnetostatic-field theory

Physical Review Special Topics - Accelerators and Beams