IEEE TRANSACTIONS ON PLASMA SCIENCE, VOL. 39, NO. 2, FEBRUARY 2011 737
Analysis on Useful Lifetime of High-Power
Closing Switch With Graphite Electrodes
Lee Li, Fuchang Lin, Cai Li, Hu Guan, Liu Ning, and Zhou Zhengyang
Abstract—High-power closing switches with graphite electrodes
have been used in power-supply system for a large laser pump.
The useful lifetime of this kind of switch is an interesting and
important issue. Previous researchers have observed that the
graphite erosion loss is proportional to the amount of transfer
charge in a high-power pulsed discharge. Therefore, the erosion
rate of graphite may be used for predicting and estimating the
electrodes’ useful lifetime. According to the mathematical model
proposed in this paper, the lifetime of a closing switch with
graphite electrodes is dependent upon several key parameters,
including the dimensions of electrode, density, the erosion rate of
graphite electrodes, undervoltage ratio, working temperature, and
the amount of energy transfer. A mathematical formula describing
the relationship between lifetime and those parameters has been
deduced. Based on a newly developed spark-gap switch which can
support over 100-C single transfer charge, this proposed lifetime
model has been verified. This paper may quantitatively perform
the function of guidance in engineering applications of graphite
electrode switches in large pulsed-power facilities.
Index Terms—Charge transfer, erosion rate, graphite electrode,
power conditioning.
I. I NTRODUCTION
H
IGH-POWER power-supply systems are necessary for
driving large laser pumps. The power-supply module is
one of the most important units in a laser pump. With the
parallel operation of multiple units, it can generate the required
pulse for the xenon flashlamps within a laser amplifier, which
lead to the high energy gain of laser beams from the amplifier.
High voltage, high current, and high-coulomb transfer clos-
ing switches play a special role in a power-supply module.
The most practical closing switches to date are spark gaps
due to their relatively simple structure, robustness, easy field
maintenance, and low cost. A typical high-current spark gap
is the ST-300A used in the National Ignition Facility. This
switch is of a two-electrode design using high-density graphite
electrodes, supports over 300-kA peak current capability with
150-C charge transfer per discharge shot, and is relatively
inexpensive and reliable [1], [2]. Its cotwin, the ST-4198 switch,
which was developed for electromagnetic launch, can operate
at a maximum peak current of 850 kA or a maximum single
charge transfer of 350 C [3]. However, the main drawback of
Manuscript received May 29, 2010; revised October 6, 2010 and
November 23, 2010; accepted November 29, 2010. Date of publication
January 17, 2011; date of current version February 9, 2011.
The authors are with the College of Electrical and Electronic Engineer-
ing, Huazhong University of Science and Technology, Wuhan 430074, China
(e-mail: leeli@mail.hust.edu.cn; fclin@mail.hust.edu.cn).
Color versions of one or more of the figures in this paper are available online
at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/TPS.2010.2097280
Fig. 1. Structure of the two-electrode spark-gap switch.
spark-gap switches is limited useful lifetime. The lifetime of
the ST-300A switch is about 1500 shots (i.e., the total charge
transfer is about 150 kC), and the ST-4198 only supports about
100 shots. It is well known that the lifetime of a spark-gap
switch is related directly or indirectly to the erosion of the
electrodes. How would one design and manufacture a spark-
gap switch with a long lifetime? In other words, what is the
mathematical principle of graphite electrode lifetime in high-
current discharge? In this paper, the erosion features of graphite
electrode are analyzed first. Then, it is proposed to use the
erosion rate to estimate the lifetime of graphite electrodes. This
paper presents a practical method of measuring and calculating
the erosion rate. Next, the mathematical model of electrode
lifetime is deduced. This model represents a series of key
parameters related to useful lifetime. Reasonable parameter
configuration will be helpful for long-lifetime design. Lifetime
testing of a spark gap with graphite electrodes verifies the
correctness of the proposed lifetime model.
II. OVERVIEW OF SPARK-GAP SWITCHES
In order to make the issue more clearly understood, the
structure of the spark-gap switch is shown in Fig. 1. The
spark-gap switch generally adopts a coaxial structure and high-
density graphite electrodes. The coaxial structure can balance
the strong magnetic force, reduce shake, and restrain the arc
channel on the center of the switch. As presented in the
ST-300A [2], the main components include two main elec-
trodes, the up and down metal electrode holders, an insulator
envelope, insulator rods, etc. There are two airports in the
down holder, which can be used for air charge and insulation
recovery of repetitive discharging. Materials eroded from the
electrodes exit the switch as a gas via air charge too. Due
to the lack of a separate trigger electrode, this switch must
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