U.S. patent number 3,664,960 [Application Number 04/793,743] was granted by the patent office on 1972-05-23 for control circuit for neutron generator tube.
This patent grant is currently assigned to National Research Development Corporation. Invention is credited to James David London Hedley Wood.
United States Patent |
3,664,960 |
Wood |
May 23, 1972 |
CONTROL CIRCUIT FOR NEUTRON GENERATOR TUBE
Abstract
In the supply circuit for an ion accelerator having an ion
source and an ion extractor electrode, the supply circuit including
an energizing supply for the ion source and a power supply for the
extractor electrode, there is provided a negative feedback loop
connected to cause the extractor electrode current to control the
energizing supply output in a sense to maintain constant the
extractor current. The described embodiment is a neutron generator
tube having a plasma ion source energized by a radio-frequency
supply.
Inventors: |
Wood; James David London Hedley
(Letchworth, EN) |
Assignee: |
National Research Development
Corporation (London, EN)
|
Family
ID: |
9798351 |
Appl.
No.: |
04/793,743 |
Filed: |
January 24, 1969 |
Foreign Application Priority Data
|
|
|
|
|
Feb 2, 1968 [GB] |
|
|
5,556/68 |
|
Current U.S.
Class: |
250/423R;
376/111; 315/297; 376/114 |
Current CPC
Class: |
H05H
3/06 (20130101); H01J 27/022 (20130101); H05H
5/00 (20130101) |
Current International
Class: |
H01J
27/02 (20060101); H05H 3/00 (20060101); H05H
5/00 (20060101); H05H 3/06 (20060101); G21g
003/24 () |
Field of
Search: |
;250/84.5,103
;315/297,57 ;313/61 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Lawrence; James W.
Assistant Examiner: Frome; Morton J.
Claims
I claim:
1. A supply circuit for an ion accelerator having an ion source and
an ion extractor electrode, said circuit including an energizing
supply for the ion source, means for providing a fixed accelerating
voltage and a power supply for the extractor electrode, wherein
said circuit comprises a negative feedback loop connected to cause
the extractor electrode interception current to control the
energizing supply output in a sense to maintain constant said
extractor interception current at a small fraction of the total
current.
2. A circuit as claimed in claim 1 wherein the energizing supply is
a radio-frequency supply adapted to energize a plasma ion
source.
3. In combination, an ion accelerator having an ion source and an
ion extractor electrode, and a supply circuit for said ion
accelerator, said circuit including an energizing supply for the
ion source, means for providing a fixed accelerating voltage and a
power supply for the extractor electrode, wherein said circuit
comprises a negative feedback loop connected to cause the extractor
electrode interception current to control the energizing supply
output in a sense to maintain constant said extractor interception
current at a small fraction of the total current.
4. A combination as claimed in claim 3 wherein the ion source is a
plasma ion source and said energizing supply is a radio-frequency
supply.
5. A combination as claimed in claim 3 wherein the ion accelerator
is a sealed neutron generator tube and the ion source is adapted to
produce hydrogen isotope ions.
Description
BACKGROUND OF THE INVENTION
This invention relates to supply circuits for ion accelerators, in
particular for neutron generators in which deuterium and/or tritium
ions are extracted from a plasma and accelerated on to a target
containing deuterium and/or tritium. A neutron generator tube of
this kind is described in our UK Specification No. 1,088,088.
Briefly, in the latter generator a plasma is produced in the ion
source portion of the tube by a surrounding coil energized by a
radio-frequency oscillator. This portion of the tube is bounded by
an apertured boundary electrode, and the plasma is intensified in
the region of this aperture by an axial magnetic field derived from
a coaxial solenoid.
Positive ions are extracted from the plasma by a negative potential
applied to an extractor electrode. A plasma boundary is formed with
its perimeter keyed to the edge of the boundary electrode. The ions
are extracted into a beam whose profile depends on the electric
field configuration produced between this plasma boundary and the
potential applied to the extractor. The shape of the boundary and
its effect on beam profile depend on the plasma ion density and the
value of the applied potential. Optimum operation requires that the
ion beam pass through the extractor aperture with minimum
interception to prevent undue heating or sputtering of the
extractor electrode. The ion beam once through the extractor
aperture is accelerated through a target shield aperture by a large
negative potential applied thereto, and finally passes through the
field-free region inside a suppressor electrode to impinge on the
target.
In such tubes there is a small interception of the beam by the
extractor electrode under normal running conditions, giving rise to
an extractor current. If the interception is too great, the
extractor temperature rises and adsorbed gas is released into the
tube. This creates an unstable condition, as described in more
detail hereafter, which can result in the destruction of the tube.
It is particularly likely to occur under start-up conditions, as
the extractor potential and radio-frequency power supply to the
plasma are increased progressively.
It is an object of the present invention to provide a form of
supply circuit which alleviates this problem.
SUMMARY OF THE INVENTION
According to the present invention, in a supply circuit for a
particle accelerator having an ion source and an ion extractor
electrode, said circuit including an energizing supply for the ion
source and a power supply for the extractor electrode, there is
provided a negative feedback loop connected to cause the extractor
electrode current to control the energizing supply output in a
sense to maintain constant said extractor current. The energizing
supply may be a radio-frequency supply adapted to energize a plasma
ion source.
The present invention also provides, in combination, an ion
accelerator having an ion source and an ion extractor electrode,
and a supply circuit for said ion accelerator, said circuit
including an energizing supply for the ion source and a power
supply for the extractor electrode, wherein said circuit comprises
a negative feedback loop connected to cause the extractor electrode
current to control the energizing supply output in a sense to
maintain constant said extractor current. The ion source may be a
plasma ion source and said energizing supply a radio-frequency
supply.
The ion accelerator may be a sealed neutron generator tube, the ion
source being adapted to produce hydrogen isotope ions.
DESCRIPTION OF THE DRAWING
To enable the nature of the present invention to be more readily
understood, attention is directed, by way of example, to the
accompanying drawings wherein
FIG. 1 is a schematic diagram of a neutron generator tube connected
in a supply circuit embodying the present invention.
FIG. 2 is a graph showing the variation of extractor and total tube
current with extractor voltage at constant RF power.
FIG. 3 is a graph showing the variation of total tube current with
extractor voltage when the RF power is controlled in accordance
with the present invention.
DESCRIPTION OF THE PREFERRED EMBODIMENT
FIG. 1 shows a neutron generator tube of the kind described in
detail in UK Specification No. 1,088,088. It comprises an
ion-source portion 1 surrounded by an RF coil 2 to energize a
plasma therein, and a magnetic solenoid 3. At one end is a backstop
4 and at the other an apertured boundary electrode 5, beyond which
are successively an extractor electrode 6, a shield electrode 7, a
suppressor electrode 8, and a target 9. The cross-section of the
ion beam under normal working conditions is indicated approximately
at 10. The gas pressure is maintained constant by a replenisher
controlled by a Pirani gauge, both of which are omitted from FIG. 1
for clarity, as is part of the tube envelope. FIG. 1 also shows the
connections from the associated supply circuit.
Typical preferred operating conditions for the tube are as
follows:
Gas pressure (50/50 D/T mixture) (P) 1.2.times.10.sup..sup.-2 Torr
RF energizing power (W) 200 watts RF frequency 14 MHz Magnetic
field (H) 90 gauss Extraction potential (V.sub.E) 4.5 kV Extraction
interception current (I.sub.E) 0.1 mA Acceleration potential
(V.sub.T) 120 kV Total tube current (I.sub.A) 12 mA Target current
(I.sub.T) 6 mA Suppressor voltage (V.sub.S) 440 V Suppressor
current (I.sub.S) 6 mA Ion beam diameter at target 2.8 cm Neutron
output 10.sup.11 neutrons/ second
FIG. 2 illustrates a typical extractor control characteristic for a
constant RF energizing power W. With increasing extractor potential
V.sub.E, the interception current I.sub.E first rises to a peak
corresponding to increasing ion extraction accompanied by beam
collection by the extractor. Subsequently ion extraction continues
to increase but is associated with a repression of the plasma
boundary into the ion-source portion of the tube, the effect of
which is closer beam focussing so that the beam passes through the
extractor aperture and the interception current falls. The beam
profile is well defined with a small interception on the extractor,
and this in turn defines the ion beam diameter at the target.
The effect of increasing the RF power W is to shift the whole
characteristic to the right as shown. This effect is due to
increased ion-source plasma density, which tends to bring the
plasma boundary forward into the extraction region and requires an
increased extraction potential to restore the initial focus
conditions and so reduce the interception current.
A whole series of these characteristics exists, corresponding to
the range of possible RF powers, but at the higher levels they are
impossible to determine because of instabilities caused at high
values of I.sub.E. The maximum continuously acceptable value of
I.sub.E is about 0.15 mA.
Increase beyond this firstly causes a rise in the temperature of
the extractor electrode, and in the long term, sputtering.
Sputtered material is undesirable because eventually conducting
deposits can be formed on the insulating walls of the tube with
adverse consequences to the high voltage insulation and, less
seriously, interference with ion source performance.
More serious and even catastrophic can be the chain of positive
feedback events brought about by temperature rises, as follows:
i. Adsorbed gas is driven out of the extractor.
ii. Owing to the finite response time of the pressure control
system the gas pressure rises.
iii. With increase in pressure, RF power is more readily coupled to
the ion source and the plasma ion density increases.
iv. Following the characteristics of FIG. 3, interception
increases, followed by a further temperature rise of the extractor
electrode.
v. At the same time ion current to the target increases and if
allowed to rise beyond the coolant system capacity will cause rapid
target outgassing and further rises in pressure.
vi. The electron current to the backstop also increases with
pressure and a further outgassing may ensue from that
electrode.
If this sequence is not controlled the power dissipation at the
extractor electrode may rise to such a point that the
glass-to-metal seal is destroyed. Protection could be achieved by
over-current trips in the various circuits, but this can result in
an unwelcome and unacceptable number of "shut-downs". Any variation
in the tube supply conditions may initiate this chain, and
continuous control is important for long-term stable
conditions.
In the present invention, any increase of interception current is
caused to reduce the RF power, thereby reducing the degree of
interception and so inhibiting the runaway chain of events
described above. Referring again to FIG. 1, the interception
current I.sub.E is made to flow through a resistor R.sub.E and
thereby develop a potential across it. This potential is compared
with a reference potential derived from a source 11 by a
transistorized differential amplifier 12 of conventional
construction. The output of amplifier 12 controls the firing angle
of a thyristor control circuit 13 connected in the 50 c/s mains
supply to the RF oscillator 14, and thus ultimately the RF power
supplied to the ion source. To ensure stability of the negative
feedback loop so formed, the sensitivity and time-constants are
adjusted in a manner familiar to those skilled in the negative
feedback control art. The desired value of interception current
I.sub.E is set by adjusting the value of R.sub.E.
The above-described supply circuit has enabled long-term stable
operation of the tube to be achieved, for example a 12-hour
unattended run. In the absence of the negative feedback loop, an
operator was required to be in constant attendance.
A further advantage of the invention is that the extractor
electrode can be employed as a true control grid, as illustrated in
FIG. 3. The extractor potential can be increased or decreased at
will to determine the ion current and consequent neutron output.
The necessary changes in the RF power supply to the ion source are
automatically introduced by the feedback circuit and the plasma
boundary is maintained over a wide range in the correct position
for stable formation of an ion beam of the desired profile and
hence for a stable position on the target.
Although described with reference to a neutron generator tube using
an RF plasma ion source, it will be appreciated that the present
invention can be applied to neutron generators or other particle
accelerators employing an extraction electrode, whatever the
process by which the energizing supply causes ion production in the
source. For example, in a neutron generator using a PIG-type ion
source, the extractor current can be made to control the anode
voltage and hence the discharge current in the source. Neutron
generators using such ion sources, also known as Penning sources,
are described, for example, in UK Specifications Nos. 976,664 and
980,947 and in Nucleonics, December 1960, pp.69-74.
* * * * *