[0001] This invention relates to a high voltage switch, in particular to a high pressure
gas switch for use in high voltage, high power switching applications.
[0002] High pressure gas switches are widely used in high pulse power switching. They offer
a very simple compact means of very high pulse power switching with low mass and volume.
However, known designs for such switches have a relatively limited life due to uneven
and damaging electrode wear.
[0003] Preferred embodiments of the present invention are as defined in the claims.
[0004] A switch according to preferred embodiments of the present invention has been found
to have a long operational life, despite the high voltages being switched, of the
order of several hundred kilovolts and instantaneous power levels of the order of
Gigawatts. Long operational life is characterised in this invention by even wearing
of the facing surfaces of the electrodes, so preserving the operational characteristics
of the switch, with no significant localised damage such as pitting or fracturing.
Furthermore, the switch has been found to be less sensitive to temperature variations
that may otherwise cause prior art switches to operate at reduced power levels outside
optimal temperature ranges.
[0005] Preferred embodiments of the present invention will now be described in more detail,
by way of example only, and with reference to the accompanying drawings of which:
Figure 1 is a sectional view through a high pressure gas switch according to a preferred
embodiment of the present invention;
Figure 2 is a sectional view through an electrode of a first preferred design in the
present invention;
Figure 3 provides sectional views through an electrode pair according to a second
preferred design in the present invention;
Figure 4 is a simplified representation of the electrode configuration of the switch
in Figure 1;
Figure 5 is a plot of the electric field enhancement arising in the simplified electrode
arrangement in Figure 4;
Figure 6 is a simplified representation of the electrode configuration of a the switch
using the electrode pair shown in Figure 3; and
Figure 7 is a plot of the electric field enhancement arising in the simplified electrode
arrangement in Figure 6, with the plot of Figure 5 shown for comparison.
[0006] A simple high pressure gas switch according to a preferred embodiment of the present
invention will now be described with reference to Figure 1. The switch may be used
in a number of different applications, preferably those requiring the switching of
voltages of the order of several hundred kilovolts at high instantaneous power levels,
but at relatively low overall energy levels. Such applications are in contrast to
switching in X-ray apparatus, for example, in which voltages of the order of megavolts
or higher need to be switched, with high overall energy levels.
[0007] Referring to Figure 1, a sectional view through the preferred high pressure gas switch
100 is shown. The switch 100 comprises a high pressure containment vessel 105, preferably
made from a high strength metal such as stainless steel and in the shape of a cylinder.
Insulating members 110, preferably made from ceramic or a plastic such as nylon or
polypropylene, serve both as the end walls of the high pressure containment vessel
and to electrically isolate the respective electrode 115, 120 from the cylindrical
brass portion 105 of the vessel. Sealing rings 125 are provided to seal the vessel
when in its assembled state with the insulating members 110 held securely in place
by a number of bolts 130. The containment vessel provides a void 135 around the electrodes
for holding a suitable gas, preferably nitrogen, hydrogen or SF
6, under very high pressure, preferably in the range of 300psi to 1200psi.
[0008] The electrodes 115, 120 are held in a fixed position by the insulating members 110
so that there is a nominal gap D between the electrodes 115, 120. Electrical connection
to each of the electrodes 115, 120 is by means of an access hole 140 created in the
respective insulating member 110 to expose a connecting portion 145 of the respective
electrode 115, 120. Electrical connection to the electrodes 115, 120 is by any of
a number of possible configurations, for example by means of a push-fit sleeve that
may fit tightly around a slightly narrowed portion of the connecting portion 145 to
ensure a reliable electrical connection. However, preferably, any such electrical
connections may be additionally soldered or otherwise bonded for extra reliability
appropriate to the voltage levels intended for this switch 100.
[0009] Preferred designs and advantageous features of the electrodes 115, 120 will now be
described in more detail with reference, in particular, to Figure 2 and to Figure
3 .
[0010] Referring firstly to Figure 2, a sectional view is provide through an electrode 200
of a first preferred design, with dimensions shown in millimetres. The electrode 200
is made preferably of brass and comprises a facing surface 205 having a flat central
region 210 surrounded by a raised annular region 215. The radius of curvature of any
rounded surface of the raised annular region 215 is relatively small in comparison
with the intended width of the electrode 200 so that the raised surface features on
the facing surface 205 serve to increase the surface area of the electrode over which
erosion takes place. Furthermore, as will be discussed below, the radius of curvature
of the raised surface features is made significantly less than the intended electrode
separation so that the area over which field enhancement and hence enhanced erosion
takes place is increased. The raised features 215 according to these preferred design
considerations has been found to contribute to the extended operational life of the
switch 100 according to preferred embodiments of the present invention.
[0011] Whereas this first preferred design may be used for both of the electrodes 115, 120,
substantially as shown in the example of Figure 1, the advantages of long operation
life for a switch employing this first design of electrode 200 has been found to be
preserved even though one of the electrodes is provided with an entirely flat facing
surface 205. After a long period of operation of a switch 100 made according to this
design, the initially flat facing surface has been found to have a shallow annular
depression formed corresponding to the shape and position of the raised annular portion
215 of the opposite electrode. This has the effect of preserving or, in the case of
an initially flat electrode, enhancing the degree of similarity in the profiles of
the facing surfaces of the electrodes so as to maintain a substantially even gap between
the electrodes and hence to maintain substantially even wear over their facing surfaces.
[0012] Referring now to Figure 3, in particular to Figure 3a, a second preferred design
for a negative, or high voltage (HV) electrode 300 is shown as a sectional view with
dimensions indicated in millimetres. In this second design, the facing surface 305
of the electrode is provided with an outer raised annular region 310 and a concentrically
arranged inner raised annular region 315, with flat regions in between to give a "corrugated"
facing surface 305 to the electrode 300. The preferred design for a corresponding
positive, or ground electrode 350 is shown in sectional view in Figure 3b to have
a simple plane facing surface 355. As discussed above and as will be analysed further
below, it has been found that the advantages of even electrode wear are preserved
or indeed enhanced by the use of an initially flat electrode 350 in association with
the electrode of the first (200) or second (300) preferred electrode design.
[0013] Whereas the first and second preferred electrode designs described above use continuous
raised annular portions, in a further preferred embodiment of the present invention
an arrangement of discrete "mounds" may be provided across the facing surface of the
HV electrode, rather than using one or more annuli. Each mound may have a similar
radius of curvature to that of the annular portions in the first and second designs.
However, advantageously, an arrangement of discrete mounds may provide a greater facing
surface area for an electrode than that provided using continuous annuli and this
feature is likely to contribute to extended electrode life.
[0014] A switch 100 according to preferred embodiments of the present invention, using electrodes
of the preferred designs described above, is operated by applying a voltage across
the electrodes 115, 120 which increases the electric field within the high pressure
gas until breakdown occurs. The discharge following breakdown is a narrow plasma channel
across the gap between the electrodes 115, 120. It has been observed that the breakdown
channel predominantly occurs at points over the raised surface of an annulus or a
discrete mound on the facing surface where the electric field strength is enhanced.
However, surprisingly, the observed evenness of electrode wear over the raised surface
features in particular, despite use of an initially flat-faced opposing electrode,
suggests that breakdown occurs randomly at any point over the raise surface, not just
that region at the apex of the raised surface for which the initial gap between electrodes
is a minimum.
[0015] In a typical experiment, following a long period of operation of the switch 100 of
the order of 100x10
6 switching shots, using the first preferred design of electrode 200 for the high voltage
electrode and a flat-faced electrode for the ground electrode, each of dimensions
indicated in the respective figures, the radius of the raised annular region 215 of
the high voltage electrode 200 was reduced by 0.26mm from nominal and the flat central
region 210 was eroded 0.4mm from nominal. The flat-faced ground electrode was also
eroded and an annular depression, 0.2mm deep, of substantially the same sectional
profile as the raised annular region of the high voltage electrode, was worn in its
flat facing surface.
[0016] During breakdown, the plasma channel diameter is small and its inductance is significant,
thereby limiting the rate of rise of current through the switch 100. The electrical
breakdown strength of the gas contained in the switch 100 increases almost linearly
with pressure. Preferably, high gas pressure is used so that the required gap between
the electrodes and hence the plasma channel length is substantially minimised. A reduced
plasma channel length enables faster current rise and hence reduced switching time.
Preferably, the gas contained in the switch 100 is at a pressure of between 300psi
and 1200psi.
[0017] A further advantageous feature of a switch 100 according to preferred embodiments
of the present invention described above is an observed reduced temperature dependence
when the switch is used in a pulsed charge application. Conventionally, the breakdown
voltage between electrodes of the switch is a function not only of gas pressure but
also of gas temperature. Where, as in preferred embodiments of the present invention,
a very high gas pressure is used, preferably in excess of 500psi, if the gas switch
100 is charged in the first microsecond to a very high field strength, the breakdown
voltage of the switch has been observed to become predominantly a function of the
plasma channel formation time, rather than of gas temperature and pressure. This property
is exploited in such applications to reduce the switch dependence on gas pressure/
temperature, so increasing the temperature range over which the switch 100 operates
at the required power levels.
[0018] A simplified analysis will now be provided to describe the principles of operation
of a switch 100 according to preferred embodiments of the present invention. This
analysis will be made with additional reference to figures 4 to 7.
[0019] Referring firstly to Figure 4, and considering the arrangement of electrodes shown
in particular in the switch 100 of Figure 1, the electric field across the gap between
the raised annular regions of the electrodes 115, 120 can be estimated by considering
the electric field between two conducting cylinders 400, 405 of radius R and separation
D.
[0020] For an applied voltage of V volts between the cylinders 400, 405 the maximum electric
field strength is given by the equation:

[0021] If a plane field existed within the gap, the electric field would be simply V/D (volts/metre).
Preferably, the annular gap is designed such that the radius of the annulus, R, is
smaller than the gap separation, D. In this situation, the maximum electric field
is increased according to the equation:

[0022] A plot 500 of the enhanced E-Field is shown in Figure 5. As can be seen from the
plot 500 in Figure 5, where R<<D the maximum electric field tends to become independent
of the gap separation D.
[0023] Since the electric field is enhanced at the annular radius, R, and breakdown can
be observed to occur at that radius, then spark erosion would be expected to be concentrated
at the radius. However, surprisingly, in the switch 100 of the present invention,
it has been observed that erosion occurs much more evenly across the spark gap facing
surfaces.
[0024] For the preferred embodiments of the present invention in which there is one flat-faced
positively charged electrode, the situation may be represented in a simplified diagram
as shown in Figure 6. A cylinder 600 of radius R is placed a distance D from a flat-faced
electrode 605. In that arrangement, the maximum field strength is given by the equation:

[0025] A similar plot of the enhanced field due to the radius of the annular gap is shown
in Figure 7. Referring to Figure 7, the plot 700 for the "single-ended" switch arrangement
of Figure 6 is provided along with the plot 500 for the "double-ended" switch arrangement
from Figure 4 and Figure 5, for comparison. As can be seen from Figure 7, a greater
enhancement is achieved with the single-ended switch arrangement, which advantageously
is also simpler and cheaper to produce.
[0026] Thus, the analysis supports the observation referred to above that the use of one
flat-faced electrode and one "radiused" electrode in preferred embodiments of the
switch 100 provides for increased field enhancement and hence reduced dependence upon
electrode separation (which increases slightly as the electrodes wear). The use of
a "corrugated" or discretely mounded facing surface for the HV electrode increases
the surface area of the eroding face of the electrode and hence increases its operational
life. The surprisingly even wear of the electrodes in this geometry works in tandem
with the increased tolerance of electrode separation to further increase the operational
life of the electrodes and hence of the switch 100. The use of brass as an electrode
material, rather than a harder metal such as copper tungsten, has been observed to
contribute to more even electrode wear in that the harder metals appear to be more
susceptible to significant pitting than brass at the voltage, power and energy levels
for which the present invention is preferably directed.
[0027] A yet further advantage, mentioned above, arises from operation of the switch 100
at the highest practical pressures, preferably in the range 300psi to 1200psi, but
more preferably in excess of 500psi. This enables the switch 100 to be operated in
such a way as to increase the range of operational gas temperatures (and hence pressures)
for which the switch 100 is able to switch at full design power.
[0028] Further designs for electrodes, following the principles described in preferred embodiments
of the present invention above, would be apparent to a person of ordinary skill in
this field and would fall within the scope of the invention as defined in the claims.
1. A switch, comprising:
a containment vessel for holding a gas at high pressure;
first and second electrodes housed within the containment vessel and electrically
isolated therefrom;
wherein the first and second electrodes are supported in a face-to-face arrangement
whereby the facing surfaces of the first and second electrodes are separated by a
nominal distance D and the facing surface of at least one of the first and second
electrodes comprises at least one portion that is raised in comparison with the remainder
of the facing surface.
2. The switch according to Claim 1, wherein the at least one raised portion comprises
a raised annular region.
3. The switch according to Claim 1 or Claim 2, where the at least one raised portion
comprises a plurality of raised annular regions arranged over the facing surface.
4. The switch according to Claim 3, wherein said plurality of raised annular regions
are arranged concentrically.
5. The switch according to Claim 1, where the at least one raised portion comprises a
plurality of locally raised regions distributed over the facing surface.
6. The switch according to any one of the preceding claims, wherein the at least one
raised portion comprises a rounded surface.
7. The switch according to Claim 6, wherein the radius of curvature of the rounded surface
is significantly less than the separation distance D of the first and second electrodes.
8. The switch according to any one of the preceding claims, wherein the containment vessel
contains a gas at a pressure in the range 300psi to 1200psi.
9. The switch according to Claim 7, wherein the pressure of the gas is at least 500psi.
10. The switch according to any one of the preceding claims, wherein one of the first
and second electrodes is provided with a substantially flat facing surface.
11. The switch according to any one of the preceding claims, wherein at least one of the
first and second electrodes is made from brass.