U.S. patent number 3,899,681 [Application Number 05/457,673] was granted by the patent office on 1975-08-12 for electron beam device.
This patent grant is currently assigned to The United States of America as represented by the United States Energy. Invention is credited to Everet H. Beckner, Milton J. Clauser.
United States Patent |
3,899,681 |
Beckner , et al. |
August 12, 1975 |
Electron beam device
Abstract
An electron beam device in which a hollow target is
symmetrically irradiated by a high energy, pulsed electron beam
about its periphery and wherein the outer portion of the target has
a thickness slightly greater than required to absorb the electron
beam pulse energy.
Inventors: |
Beckner; Everet H.
(Albuquerque, NM), Clauser; Milton J. (Albuquerque, NM) |
Assignee: |
The United States of America as
represented by the United States Energy (Washington,
DC)
|
Family
ID: |
23817686 |
Appl.
No.: |
05/457,673 |
Filed: |
April 1, 1974 |
Current U.S.
Class: |
376/152; 376/101;
376/105 |
Current CPC
Class: |
H05H
1/22 (20130101); Y02E 30/10 (20130101) |
Current International
Class: |
H05H
1/22 (20060101); H05H 1/02 (20060101); G21b
001/00 () |
Field of
Search: |
;176/1,8,93
;250/499,500,501,502,439 ;313/61 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Dixon; Harold A.
Attorney, Agent or Firm: Carlson; Dean E. King; Dudley W.
Constant; Richard E.
Claims
What is claimed is:
1. An electron beam device comprising a target consisting
essentially of a hollow shell of an electron absorbing material,
said shell having a thickness to diameter ratio of from about 1 to
5 to about 1 to 50, a thickness of from about 0.1 to 1.0 mm
sufficient to absorb in outer portions of said shell substantially
all electrons impinging on the shell, and hydrogen isotope disposed
in the interior thereof; and means adjacent and generally
encircling said shell for producing a high energy pulse beam of
electrons circumferentially encompassing and focused on and
substantially encircling said target for accelerating inner
portions of said shell inwardly against said hydrogen isotope.
2. The device of claim 1 wherein said electron beam producing means
includes a diode discharge means for generating a pulsed electron
beam having voltage of from about 0.5 to 5 megavolts of from about
5 to 20 nanoseconds in duration.
3. The device of claim 1 wherein said hydrogen isotope is selected
from the group consisting of deuterium and tritium and mixtures
thereof with from about 10 to 1,000 micrograms of isotope.
4. The device of claim 3 wherein said deuterium and tritium are
present in about equal atomic concentrations.
5. The device of claim 1 wherein said shell is of sufficient
thickness to block substantially all of said electrons from said
hydrogen isotope.
6. The device of claim 5 wherein said shell includes an outer layer
for absorption of said electron beam and an inner layer for
acceleration against said hydrogen isotope.
7. The device of claim 1 wherein said target is spherical in
shape.
8. A target for use in an electron beam device consisting
essentially of a hollow spherical shell of an electron absorbing
material, said shell having a thickness to diameter ratio of from
about 1 to 5 to about 1 to 50, a thickness of from about 0.1 to 1.0
mm sufficient to absorb substantially all electrons impinging on
the shell from said device, and hydrogen isotope disposed in the
interior thereof.
Description
BACKGROUND OF INVENTION
Many more techniques and devices are being developed in order to
produce high energy plasmas and other materials which may result in
fusion or the like, or to be used for material studies, testing of
deposition of high energy in materials or for similar purposes. One
such technique or device is high intensity electron beam generating
machines. Such machines are being built or developed which are
capable of producing electron beams in pulses having currents of
from about 100,000 to greater than 1,000,000 amperes at voltages of
from about 100,000 volts to greater than 10,000,000 volts in time
periods of 100 nanoseconds or less.
In order to achieve the desired interactions and reactions of the
materials to achieve these purposes, the electron beam device
should desirably focus this beam energy to a very small point or
space in a symmetrical or uniform manner. This is particularly true
in plasma and fusion-type applications where an amount of material
to be ionized or fused must be heated to very high temperatures in
the neighborhood of from about 10.sup.5 to 10.sup.8 .degree.C and
compressed to extremely high densities. It has been found to be
difficult to achieve desired high energy electron beam or beams
having suitable energy and pulse durations and then to focus the
so-produced electron beams to a desired size which may be absorbed
in a time period and configuration which would produce
significantly high density and high temperature plasmas and/or
fusion.
Attempts to achieve nuclear fusion with an electron beam are
referred to by Rudakov and Samarsky in the Proceedings of the 6th
European Conference on Controlled Fusion and Plasma Physics,
July-August, 1973, at pages 487-490, wherein an electron beam would
be directed against a target from one side with the target and beam
parameters selected to have the beam penetrate target and enclosed
fuel material to the targets' far side. Interior portions of the
target would be vaporized and the vapor accelerated against the
fuel material. The vapor would be to act as a relatively hot, low
density tamping material which might not be effective in producing
the levels of fuel compression desirable in many fusion and plasma
applications.
SUMMARY OF INVENTION
In view of the above, it is an object of this invention to provide
an electron beam device which includes a target capable of
absorbing and utilizing a high energy electron beam pulse for
symmetrical compression thereof.
It is a further object of this invention to provide an electron
beam device which may deposit a high energy, electron beam pulse
into a spherical target in nanosecond time periods at high
energies.
It is a further object of this invention to provide a novel
electron beam implosion target.
Various other objects and advantages will appear from the following
description of the invention, and the most novel features will be
particularly pointed out hereinafter in connection with the
appended claims. It will be understood that various changes in the
details, materials and arrangements of the parts, which are herein
described and illustrated in order to explain the nature of the
invention, may be made by those skilled in the art.
The invention comprises a target composed of an outer hollow shell
of electron beam absorbing material having a thickness to diameter
ratio of about 1 to 10 or 20 and a material enclosed within the
shell which it is desired to implode, and means for producing a
high energy electron beam pulse deposited in the outer surface of
the target for vaporizing outer portions of the shell and for
imploding inner portions of the shell against the enclosed
material.
DESCRIPTION OF DRAWING
The invention is illustrated in the accompanying drawing
wherein:
FIG. 1 is a partially cutaway view of a target including the
features of this invention;
FIG. 2 is a cutaway and somewhat diagrammatic view of an electron
beam device which may be utilized to irradiate the target
illustrated in FIG. 1;
FIG. 3 is a graph illustrating the effects produced by electron
beam irradiation of the target of FIG. 1; and
FIG. 4 is an elevation view of an alternate target and anode
arrangement which may be utilized in the device of FIG. 2.
DETAILED DESCRIPTION
The target 10 which may be utilized in the electron beam device of
this invention is illustrated in FIG. 1. Target 10 includes a
hollow spherical shell 12 which is formed of an appropriate
material of prescribed shell thickness and diameter. The shell
material should be such that will efficiently absorb a beam of high
energy electrons. For example, the shell material may be made of a
high density material having a density of from about 15 to 20 grams
per cubic centimeter, such as gold, tungsten and uranium or the
like and alloys with these materials, or an appropriate electron
absorbing lower density material, such as lead, iron or the like.
The shell 12 must be formed with proper thickness and diameter to
absorb substantially all of the electron beam energy before the
electron beam pulse terminates and the shell is ablated and
imploded. The shell 12 wall thickness should be great enough to
prevent or block substantially all of the electrons from
penetrating the shell into its interior. It has been found that the
shell thickness and shell outer diameter should be at a ratio of
from about 1 to 5 to about 1 to 50, preferably about 1 to 10 or 20,
with the shell thickness being in the range of from about 0.1 to
1.0 millimeters and the outer shell diameter in a range of from
about 1 to 10 millimeters. A shell 12 made of the above mateials,
and particularly the high density materials, with these dimensions
will efficiently absorb the electron beam energy in outer portions
of the shell and act as a pusher by accelerating essentially cold,
high density material inwardly to compress and heat the fuel and
further function as a tamper during burning of the fuel.
The interior portion 14 of shell 12 may include hydrogen isotope
fuel in an appropriate form which is substantially shielded from
the electrons in the electron beam by shell 12. For example, the
hydrogen isotope may be a gas, liquid, or solid or be in compound
form with such as lithium or carbon. The hydrogen isotope may be
either deuterium or tritium or a mixture of the two isotopes. As a
mixture, the deuterium and tritium may be at about equal atomic
concentrations (e.g., 40% deuterium and 60% tritium by weight). It
is desirable, for effective utilization, that the hydrogen isotope
by present in portion 14 of shell 12 with about 10 to 1,000
micrograms of isotope.
The shell 12 may be formed of a single material as shown, or it may
be in discrete layers of different materials which will provide
enhanced operation of the respective functions of the shell. For
example, the shell 12 may include an outer layer which is highly
efficient in absorption of electron beam energy with one or more
inner layers which function better as pushers for compression of
the fuel in portion 14 and as a tamper during fuel ignition and
burning. For example, the shell segment 12a shown in FIG. 1a may
include an outer layer 16 which is most effective as an electron
beam absorber and an intermediate or inner layer 18 of gold or
tungsten or the like which functions more effectively as a pusher
and tamper material during fuel compression and burning.
In order to provide the desired electron beam absorption, pushing
and tamping in target 10, the target 10 must be irradiated by a
high energy and short duration electron beam pulse having voltage
of from about 0.5 to 5 megavolts, energy of from about 0.1 to 10
megajoules, power of from about 10.sup.13 to 10.sup.15 watts, and
duration of from about 5 to 20 nanoseconds. In addition, the
electron beam pulse having these characteristics should be directed
against the target 10 in a generally symmetrical, focused manner
substantially encompassing and encircling the outer surface of the
target 10. It has been found that such may be achieved by using a
diode-type of discharge in an arrangement as illustrated in FIG. 2
with a diode electron beam generator having an impedance below or
about 10 ohms and an inductance below or about 1.0 nanohenry. In
the arrangement of FIG. 2 the target 10 may be positioned in an
appropriate manner generally at the center of a circular,
disc-shaped anode electrode 22 intermediate the cylindrical cathode
electrodes 24a and 24b. Anode 22 may be in the form of a thin sheet
or foil or be a vapor or plasma and may be provided with an
aperture or other position for receiving or holding target 10. It
has been found that the anode 22 and cathodes 24a and 24b should
have a diameter to discharge gap width ratio of greater than 10 to
1 in order to provide the above recited impedance and inductance
characteristics. In addition, a plasma discharge may be produced
near the axis of the anode and cathodes and therebetween in an
appropriate manner, such as by vaporizing a wire, plasma injection
or the like, to provide space charge neutralization to enhance beam
pinching and further reduce impedance levels. The anode 22 and
cathodes 24a and 24b may be energized by an appropriate high energy
and high switching speed power supply 26 by a suitable control
device 28. The power supply 26 may include a capacitor energy
storage bank with appropriate high speed switching mechanisms,
explosive driven high energy electrical generator, or the like.
Another diode-type electron beam discharge device which may be
utilized is such as is described in U.S. Pat. No. 3,760,286
entitled "Electron Beam Generator" by John G. Kelly and issued
Sept. 18, 1973. Other types of single or multiple electron beam
generating apparatus may be utilized which will produce the desired
irradiation of the target 10. If it is desired, a single cathode
and anode may be employed for some operations where less uniform
electron beam discharges may be utilized.
A combination of target parameters and electron beam
characteristics to provide operation in accordance with this
invention may include a target having an outside diameter of about
4 millimeters and a shell thickness of about 0.75 millimeters using
a 3 megavolt electron beam pulse having a duration of about 15
nanoseconds.
When the energy stored in power supply 26 is appropriately coupled
to the anode 22 and cathodes 24a and 24b across dischage regions or
gaps 30a and 30b, the electrons may be symmetrically emitted from
the discharge surfaces of cathodes 24a and 24b towards anode 22
along the paths indicated by lines 32a and 32b. Because of the
arrangement of the electrodes 22, 234a and 24b, the electrons will
travel along paths 32a and 32b radially inward towards the center
or axis of anode 22 and cathodes 24a and 24b from all directions
and portions of the discharge surfaces of cathodes 24a and 24b,
principally from the outer perimeter of cathodes 24a and 24b, as
shown, and will be pinched and focused by forces produced in the
beams so as to impinge against and encircle target 10 in a
relatively uniform manner about its outer surface. The
self-pinching of the electron beam results in a large spread in
angles of the beam electrons incident on the target 10 which causes
them to behave like a high temperature electron gas. The outer
surface and portions of pellet 12 will ablate and vaporize under
the influence of the electron beam and drive inner portions of the
shell 12 inward to implode the same against the fuel incorporated
in portion 14. The implosion may heat and compress the fuel and
cause ingnition thereof. During the burning of the fuel, the
remaining portions of the shell 12 will serve as a tamper to hold
the fuel compressed for a period of time to insure consumption of a
substantial fraction of the fuel.
FIG. 3 illustrates these effects graphically on a target which is
irradiated with an about 0.75 megavolt electron beam having a power
of about 1.5 .times. 10.sup.14 watts and about 0.9 megajoules of
energy. The target is a gold shell 1.8 mm in diameter and 0.15 mm
thick and encloses about 14.5 micrograms of a 50-50
deuterium-tritium mixture. Outer portions of the shell will be
vaporized and expand as indicated by curve 40 when the target is
irradiated beginning at time zero. Portions of the shell generally
to the inner limit of energy deposition, as indicated by the curve
42, will be vaporized and will then produce a shock wave, depicted
by curve 44, and drive the remaining unvaporized inner portions of
the shell inward against the fuel mixture. The inner surface of the
shell, e.g., the shell-fuel mixture interface, will follow the
curve 46. The high pressure region produced in the shell from
electron beam absorption, together with the shock wave, pushes the
inner portion of the shell inward to compress and heat the fuel
mixture. The maximum compression may occur at near 8.7 nanoseconds
after which a neutron pulse, such as pulse 48, may be produced
having an amplitude related to the compression and temperature
achieved in the fuel mixture.
If it is desired to provide repetitive operation of the device
shown in FIG. 2, after ignition and burning of the target 10, the
control device 28 may release or otherwise inject additional
targets, such as additional targets 10' and 10" in tube 34, in an
appropriate manner into the discharge regions 30a and 30b between
anode 22 and 24 at the center of anode 22. For example, the targets
10' and 10" may be held magnetically within tube 34 and be released
one at a time upon receipt of suitable control signals from the
control device 28 and dropped by gravity through an appropriate
passageway 36 in cathode 24a into the discharge regions. When the
so released target reaches the desired central position on anode
22, the control device 28 may then initiate power supply 26 to
provide another electron beam pulse discharge against the new
target. For applications using a solid anode 22, the anode can be
formed as a rotating disc 22' or as a sliding or otherwise moveable
elongated sheet (now shown) with multiple targets 10, 10' and 10"
positioned therein, as shown in FIG. 4. The targets may then be
sequentially rotated about shaft 38 into the position shown in FIG.
2. Any number of targets may be supported on disc 22' within the
limits of the discharge dimensions between cathodes 24a and 24b and
the diameter of anode 22'.
It will be understood that the preferred spherical shaped target 10
may be varied to other configurations or the thickness of shell 12
varied to tailor the target to provide a uniform compression of the
fuel material. For instance, the target 10 may have an ovate or
elliptical shape which may be positioned in a suitable manner into
a desired orientation with respect to the electron beam for some
electron beam generators having non-symmetrical beam shapes.
* * * * *