AU479212B2 - Process fcr extracting energy froma nuclear fusion reaction - Google Patents
Process fcr extracting energy froma nuclear fusion reactionInfo
- Publication number
- AU479212B2 AU479212B2 AU74310/74A AU7431074A AU479212B2 AU 479212 B2 AU479212 B2 AU 479212B2 AU 74310/74 A AU74310/74 A AU 74310/74A AU 7431074 A AU7431074 A AU 7431074A AU 479212 B2 AU479212 B2 AU 479212B2
- Authority
- AU
- Australia
- Prior art keywords
- energy
- fluid medium
- set forth
- fusion
- method set
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
Description
74 31 0 n4
This invention relates to the Enhancement
of Fusion Reaction and more particularly to increase
of energy of fusion by the presence of a nuclei which, upon absorption of a neutron, will disintegrate,
releasing energy.
Much work is presently being done on the
achievement of ignition and burn of fusion fuel such as, for example, deuterium-tritium in pellet form. While there are a number of different approaches to this problem, one of them includes the utilization of a source of energy from a laser and particular pellet configurations which will make it possible to achieve ignition and burn in a reaction chamber. Patents which illustrate generally the apparatus which can be used in this type of system are:
Whittlesey 3,378,446 April 16, 1968
Daiber 3,489,645 Jan. 13, 1970 Hedstrom 3,762,992 Oct. 2, 1973
It has been proposed to utilize boron in
a process and an apparatus provided for the disso-
ciation of H 2 0 in producing the components of hy-
drogen and oxygen by exposure to heutron radiation.
47 9,2 12
7 4,31 0 n in that the The present invention differs out in a region wherein the oresent process is carried exposed to the radiation process materials are directly
resulting from the fusion reaction. fusion reactor consists A general conception of a in which A central reaction chamber of two principle parts. isotopes or other nuclear nuclear fusion fuel (hydrogen is caused to fuse. An example isotopes that undergo fusion) produce fuel which will fuse to is a deuterium and tritium high neutrons produced have a helium and neutrons. The be reaction chamber, and can energy and escape the fusion in a blanket chamber, the utilized for neutron reactions between is formed by an annulus second principle part, which the outer wall. the fusion chamber and to the use of The present invention relates the fusion burn, may penetrate neutrons which, after a the range of 14 MEV neutrons reaction chamber wall in the deuterium-tritium reactions. originally derived from accord- difficult to confine, and These neutrons are very can be successfully utilized ingly, if the energy thereof to there are distinct advantages in a radiolysis process, be gained.
4 79,2 1 2
74 310 174 The reactions that appear to be most
favorable for the subject invention can be described
in the following formulation:
B1 0 Li7
Q (Energy) 2.5 MEV
Li6 t) He 4
Q 4.8 MEV
In the first reaction, B which is present
in natural boron, reacts with a neutron and releases
the energy shown above in the form of alpha radiation
and Li-7 recoil. The second reaction, Li present
in natural lithium, reacts with a neutron to release
the energy, 4.8 MEV in the form of tritium and
He-4 recoil. 6 The Li used in the latter reaction, can
be utilized, either separated, or enriched, or as
present in natural lithium.
t is thgrgfora an object of the prcont
invention to provide an apparatus and a process for
utilizing the neutrons resulting from a fusion
reaction to increase the energy by exposing them to
selected nuclei.
4 7 9,212
The present invention provides a method for
extracting energy from a fusion reaction including the step
of igniting a fusion fuel within a nuclear reaction chamber
to initiate the emission of high-energy fusion neutrons, the
method further comprising the steps of
establishing a fluid medium which includes
at least one material intimately dispersed therein containing
a constituent which dissociates exothermically upon capture
of high-energy neutrons and which functions as a neutron
moderator to modulate high-energy neutrons for efficient
reaction with said constituent and as a coolant to absorb
energy released by dissociation of said constituent,
circulating said fluid medium externally
of said reaction chamber in a region which receives high-
energy fusion neutrons when said step of igniting fusion
fuel is carried out, and
removing heat energy stored in said fluid
medium.
The features and advantages of the invention
4 7 9,2 i 2
74.310 n4
will be apparent in the following description and
claims in which the principles of operation and use
of the invention are set forth in the best mode
presently contemplated for the practice of the
invention.
A drawing accompanies the disclosure and
may be described as a schematic view of an apparatus
for accomplishing the process.
It should be appreciated that the invention
relates to the reduction of induced radioactivity in
a fusion burn by the absorption of neutrons in a medium
such as boron or lithium which react exothermically
to produce heat, but which produce no radioactive
debris. Thus, the resulting radioactivity is reduced,
the confining apparatus is less subject to deterioration,
and the entire process is easier to deal with.
In FIGURE 1, there is illustrated a laser
driven fusion reactor where a laser source 10 directs
pulse to a pellet 12 at the center of a reaction
4 7 9.2 12
7 4 31 Or by a wall 16. A pellet source chamber 14 surrounded of the fusion fuel in 18 is shown for introduction is a Surrounding the wall any suitable manner. 22 of a formed by an outer wall secondary chamber 20 resistant or other highly heat metal such as titanium fuel this chamber that the material. It is in be additional energy will materials for generating
placed. are a arrangement, there Using this general containing which boron and lithium number of ways in There are two ingredients materials may be introduced. is invention. The first required for this process metallic bearing compounds or pure boron or lithium medium for is a heat transport alloys. The second the energy derived through extracting the thermal may be A third material which nuclear reaction. the energy moderator to reduce desirable is a neutron neutron and thus improve the of the neutron flux of the composite. reaction efficiency depends upon The selection of absorber
four considerations: released the amount of energy
per neutron absorbed; after the residual radioactivity
exposure;
47 9.2 12
743 1 0 74 the neutron cross-section which is
indicative of the neutron "stopping power": and
the absorption of radiation in the
surrounding medium.
When a neutron is absorbed in any particular
isotope, the product isotopes emit energy in various
forms (alpha-radiation, beta-radiation, gamma-radiation,
neutrons, etc.). Eventually, the radiation energy is
absorbed in the medium and is converted to thermal
energy. The first consideration evaluates the efficiency
of this energy transformation. The second consideration
evaluates the rate of the energy transfer dictated
by the characteristic decay period of the products.
If the period is long, the radiation may prove a
problem from the standpoint of radiological safety.
The third consideration is the neutron cross-section
for the reaction. This determines the mass or thick-
ness of material required and, therefore, the dilution of
the energy release. The fourth consideration has to
do with the amount of absorbing medium required to
absorb the product isotope radiation. For example,
high energy gamma-radiation would require a large mass
to absorb the radiant energy. Consequently, the
energy density would be low.
4 7 9,21 2
74.310 /4 for this application The isotope preferrea neutron absorbed, energy return per should have a high produced of a long decay period no penetrating radiation
cross-..ection. Boron and lithium and a high nuclear well. meet these objectives in the fusion Other materials employed chamber between the reaction reactor annulus formed moderator material 22 are a neutron and the outer wall reaction down for efficient which slows the neutrons does not and a coolant that with boron or lithium a high neutrons, yet has parasitically capture with construc- and is compatible temperature capabilitY may also be The boron or lithium tion materials.- or ceramic metal, graphite dispersed in a solid The matrix uniform heat extraction. matrix to provide to have a low cross-section materials must also the principle competition with neutrons to avoid for the various Materials suggested neutron reaction. I. tabulated in Table applications are
4 7 9,2 12
74 310 n4 TABLE I
Dispersion Absorbers Coolants Medium Moderator
Boron Gases Water
Lithium co2 Gases Graphite Fluoride Beryllium Boron Carbide He CO 2
Lithium Hydride He Beryllium oxide
Water Aqueous solution Metal Hydride
Liquid Metals Dispersion Liquid Lithiu of Solids
Lead Solids Bismuth Aluminum Sodium Graphite NaK Beryllium oxide Fused Salts Alumina
4 7 012 1 2
74,3 1 0 [4 These additive materials which dissociate many ways. Solid exothermically can be introduced in or structures can be built to hold solid boron
lithium containing rods or plates. Provisions for
radiation periodic removal must be made to replace This can be damaged and depleted fuel elements. wall section in accomplished by providing a removable
wall 22. Part of the structure may include a neutron Any of moderator to increase the effective exposure. through a number of known coolants can be circulated to external the structure to transport thermal energy for a turbine applications (such as a steam generator or others). The electric plant, a chemical operation, the fuel in structure can be simplified by introducing salt, liquid a fluid form (aqueous solution, fused of solids, and metal, gas dispersion, fluidized bed
spherical pebbles). These forms permit continuous or
interrupting intermittent replacement of fuel without fuel handling. the reactor operation and simplifies the moderator A further simplification is to combine
and coolant into a fluid. Examples of this
and graphite- are water coolant, liquid lithium,
gas dispersions. A further simplification
47 9.2 1 2
74,310 n4 would be to combine all three functions into one
fluid, namely, a heat exchange fluid which carries,
for example, boron and also a moderator, which is
circulated through the annulus. The thermal energy
extraction and fuel replacement operations are part
of the circuit external of the reactor. The following
published sources are pertinent in connection with
this technology:
C. R. Tipton, Jr., "Reactor Handbook",
Interscience Publishers Inc., (1960).
S. Glasstone, "Principles of Nuclear
Reactor Engineering", D. Van Nostrand
Co., Inc., (1955)..
With reference to the drawing, the annulus
chamber 20 has openings 24, 26 and 30 which serve as
inlets or outlets with suitable closures.
For example, a steam or mist of H20 in
which boron is dissolved may be introduced through
openings 24 and 26 prior to a burn with an outlet
to permit proper flow. If desired, a fluid carrying
a particulate of boron or lithium may be introduced
under pressure through any of the openings. A fluidized
quantity of a particulate could be introduced at
to maintain a desired amount of boron, for example, in
the chamber 20 surrounding the reaction chamber.
4 7 9,2 1 2
74 310 With the use of a fusion reactor as a there source of neutrons to expose boron or lithium,
are a number of advantages. The unit can be operated
additive steadily with a non-destructive burn and the obtain can be supplied continuously, if desired, to There the highest efficiency of energy output. of energy will result a high neutron yield per unit boron will and the introduction of a material such as As not interfere with the operation of the reactor. product has been pointed out, there is no fission handling of radioactivity involved in the system and the
the material additions is relatively simple.
4 7 9,2 12
Claims (4)
1. A method for extracting energy from a fusion
reaction including the step of igniting a fusion fuel within
a nuclear reaction chamber to initiate the emission of high-
energy fusion neutrons, the method further comprising the
steps of
establishing a fluid medium which includes
at least one material intimately dispersed therein containing
a constituent which dissociates exothermically upon capture
of high-energy neutrons and which functions as a neutron moderator to modulate high-energy neutrons for efficient
reaction with said constituent and as a coolant to absorb
energy released by dissociation of said constituent, circulating said fluid medium externally
of said reaction chamber in a region which receives high-
energy fusion neutrons when said step of igniting fusion fuel is carried out, and
removing heat energy stored in said fluid
medium.
2. The method set forth in claim I wherein said
step includes the step of dispersing into said fluid
medium a finely-divided particulate material containing said
constituent.
3. The method set forth in claim 1 or 2 wherein
said constituent is selected from the group consisting of lithium-6 and
4. The method set forth in any one of the foregoing
claims wherein said step includes the step of dispersing
into said fluid medium a material selected from the group
consisting of water, liquid lithium, a graphite-gas
47 9.212
74. 3 1 0 4 dispersion, oari. oxide and metal hydrides to function as
said neutron moderator.
The method set forth in any one of the foregoing
claims wherein said step includes the step of dispersing
into said fluid medium a material selected from the group
consisting of carbon dioxide, helium, water and fused salt
to function as said coolant.
6. The method set forth in any one of the claims 1-4
wherein said step includes the step of dispersing into
said medium a liquid metal selected from the group consisting
of lead, bismuth and sodium to function as said coolant.
7. The method set forth in any one of the foregoing
claims wherein said fluid medium comprises a liquid, said one
material comprising a particulate material dispersed in said
liquid.
8. The method set forth in any one of the foregoing
claims wherein said fluid medium comprises a finely-divided
mist, said one material comprising a particulate material dispersed in said mist.
9. The method set forth in any one of the foregoing
claims wherein said fluid medium comprises a gas, said one mat-
erial comprising a particulate .material dispersed in said gas. A method of enhancing fusion energy substantially
as hereinbefore described with reference to the accompanying
drawings.
DATED THIS 28TH DAY OF OCTOBER, 1976.
TEXAS GAS TRANSMISSION CORPORATION By Its Patent Attorneys:
CLEMENT HACK CO. -ellows Institute of Patent Attorneys of Australia.
S4 7 9.212
74.3l 01
PFLUT 'I z~I 6
4 7-9.2Z 1 2
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US41437173A | 1973-11-09 | 1973-11-09 | |
| USUS414371 | 1973-11-09 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| AU7431074A AU7431074A (en) | 1976-04-15 |
| AU479212B2 true AU479212B2 (en) | 1976-04-15 |
Family
ID=
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CA1033317A (en) | Isotope separation process | |
| CA1026710A (en) | Electrochemical process | |
| AU7769591A (en) | Improved isotope separation process | |
| IL44946A0 (en) | High pressure infrared cell | |
| CA949447A (en) | Uranium solution mining process | |
| IE40100L (en) | Nuclear fusion reactor | |
| GB1437969A (en) | Extraction process | |
| CA1018328A (en) | Gas-preparation process | |
| CS194682B2 (en) | Process for the conversion d-glucose into d-fructose | |
| CA882667A (en) | Hot water process separation cell | |
| AU477214B2 (en) | Conversion process | |
| ZM674A1 (en) | A process for setting off and conducting micro-fission explosions for the controlled release of nuclear energy, means for carrying out the process and its application | |
| AU7431074A (en) | Process fcr extracting energy froma nuclear fusion reaction | |
| AU477267B2 (en) | Fst-neutron reactor | |
| AU488342B2 (en) | Improvements insolvent extraction process | |
| CA1024720A (en) | Hydrogen process | |
| AU493106B2 (en) | Extraction process | |
| CA987035A (en) | Migma fusion reactor | |
| AU481175B2 (en) | Reactor | |
| AU472596B2 (en) | Fast-neutron reactor | |
| AU491694B2 (en) | Electrochemical process | |
| AU475552B2 (en) | Secondary recovery method | |
| CA888105A (en) | Scrap nuclear fuel material recovery process | |
| CA1025891A (en) | Advanced cracking reactor | |
| CA1025640A (en) | Advanced cracking reactor |