The Magnetic and Electrostatic Nuclear Fusion Reactor, or simply CrossFire Fusor, is a nuclear fusion reactor whose fundamental idea was conceived in 2008 by Moacir L. Ferreira Jr., in order to overcome inherent limits of previous fusion approaches in producing fusion energy at significant rates.
Comparison to previous conceptsThe CrossFire Fusion Reactor combines features of many other fusion concepts such as Farnsworth–Hirsch Fusor[1], Bussard Polywell[2], Limpaecher Plasma Containment[3], Magnetic Mirror Machines and Penning Trap, but it differs significantly from all of them. It is most closely related to Farnsworth–Hirsch Fusor and Bussard Polywell[4][5], but it diverges from Farnsworth–Hirsch Fusor because it does not have an inner grid. It is also unlike the Bussard Polywell as it does not have recirculation of electrons while it has a well-defined voltage setup and an escape mechanism. The Polywell accelerates and confines positive ions through their attraction to negatively charged electrons, whilst the CrossFire Fusor does this using a negative voltage applied at the core region. | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| Reactants | Products | Energy Density | ||||||||||
| 1H | + 2 | 6 | Li | → | 4He + ( 3He + 6Li) → 3 4He + 1H | + | 20.9 | MeV | 153 | TJ/kg | 42 | GWh/kg) |
| 1H | + | 7 | Li | → 2 | 4He | + | 17.2 | MeV | 204 | TJ/kg | 56 | GWh/kg) |
| 3He | + | 3 | He | → | 4He + 2 1H | + | 12.9 | MeV | 205 | TJ/kg | 57 | GWh/kg) |
| 1H | + | 11 | B | → 3 | 4He | + | 8.7 | MeV | 66 | TJ/kg | 18 | GWh/kg) |
The aneutronic reactions showed above are of notable interest due to low emission of neutrons, production of charged particles in the primary reactions, that can be directly convertible into electricity.[22][9]
Examples of boron hydrides are diborane B2H6, pentaborane B5H9, and decaborane B10H14.
The following example of calculation use pentaborane (B5H9):
Electronvolt (eV) is a unit of energy and Volt (V) is a unit of electric voltage.
Electronvolt to Joule: 1 eV = 1.60218×10-19J
Electronvolt to temperature: 1 eV = 11604.505 Kelvin → 1 eV = 11604.505 K -273.15 = 11331.355 °C
Electronvolt to mass: 1 eV = 1.782662×10-36 kg → 1 MeV = 1.782662×10-30 kg
| particle | charge | mass |
| proton | +1.60218×10-19 C | 1.67262×10-27 kg |
| neutron | 0 C | 1.67493×10-27 kg |
| electron | -1.60218×10-19 C | 0.00091×10-27 kg |
11B mass= 5 protons + 5 electrons + 6 neutrons =
-
-
- 5×1.67262×10-27 + 5×0.00091×10-27 + 6×1.67493×10-27 = 18.41723×10-27 kg
-
1H mass= 1 proton + 1 electron =
-
-
- 1×1.67262×10-27 + 1×0.00091×10-27 = 1.67353×10-27 kg
-
Pentaborane (B5H9) mass: 5×18.41723×10-27 + 9×1.67353×10-27 = 107.14792×10-27 kg
Specific energy of pentaborane (eV/kg):
- 5 × (8.68MeV-123keV) / (107.14792×10-27 kg) = 3.99308×1032 eV/kg
Specific energy of pentaborane(J/kg):
- 3.99308×1032 × 1.60218 ×10-19 = 63.97633×1012 J/kg
Specific energy of pentaborane(GWh/kg):
- 63.97633×1012 / (3.6×106) = 17.77120×106 kWh/kg = 17.77120 GWh/kg
Extracting 3 electrons from pentaborane to produce positive ions:
- 107.14792×10-27 -3×0.00091×10-27 = 107.14519×10-27 kg
Charge-to-mass ratio of pentaborane(C/kg) after extracting 3 electrons:
- 3×1.60218×10-19 / 107.14519×10-27 = +4.48600×106 C/kg
The specific energy and charge-to-mass ratio are essential parameters to define the magnetic flux and electric voltages.
Using the specific energy to find the velocity of products from nuclear reaction:
- E=½mv2 → v= ((E/m) × 2)0.5 → v= ((63.97633×1012) ×2) 0.5 → v=11.31162×106 m/s
Specific impulse: 11.31162×106 / 9.80665 = 1.15346×106 s
Defining the magnet bore about 0.9 meter (0.45 meter of internal radius) and using the charge-to-mass ratio to find magnetic flux:
- r=mv/qB → r= (v/B) × (m/q) → r= (v/B) / (q/m) → B=v/(r × (q/m)) →
- B=11.31162×106 / (0.45×4.48600×106) = 5.60341 Teslas
A superconducting magnet of 6 Teslas or higher and about 0.9 meter of bore is sufficient to confine radially the plasma (reactants and products).
Calculation of a negative voltage for electrostatic acceleration of the positive ions to gain enough kinetic energy, at least 123keV, hence 550keV should be enough:
- E = q×V → V=E/q → V= (E/m)/ (q/m) →
- V= ((5×550keV×1.60218×10-19)/107.14519×10-27)/ 4.48600×106 = 916.66667×103 Volts
- Temperature: 550×103× (11604.505 K -273.15) = 6.23224 billion °C
A negative voltage of -920 kV is enough for the positive ions gain the required kinetic energy, equivalent to 6.2 billions °C.
Calculation of a positive voltage to trap longitudinally the reactants allowing the charged products to escaping. A kinetic energy choice between reactants 550keV and products 8.68MeV could be something about 1.5MeV:
- E = q×V → V=E/q → V= (E/m)/ (q/m) →
- V= ((5×1.5MeV×1.60218×10-19)/107.14519×10-27)/ 4.48600×106 = 2500×103 Volts
- V = 2500×103 - 920 kV = 1580×103 Volts
A positive voltage of 1580 kV is enough to trap the reactants allowing the products to escape.
The consumption of a fusion reactor at power of 500MWatts using a fuel with specific energy of 63.97633×1012J/kg:
- 500MW = 500×106 J/s → 500×106 J/s / 63.97633×1012 J/kg = 7.81539×10-6 kg/s
A fuel consumption of 7.82 milligrams per second is enough for producing 500MWatts.
- Ion source current: 7.81539×10-6 kg/s × 4.48600×106 C/kg = 35.05989 C/s
The ion source must provide a current of at least 35.1 Amperes for producing 500MWatts.
Cyclotron frequency: f= qB/ (2πm) = (q/m) × (B/2π) = 4.48600×106 × 6/ (2×3.14159) = 4.28382 MHz
Magnetic pressure: pm = B2/2µ° = 62/ (2×4π×10-7) = 14.32394×106 J/m3
- 14.32394×106 / 101325 = 141.36634 atmospheres
See also
- Magnetic Confinement
- Inertial Electrostatic Confinement
- Alternating-gradient focusing
- Particle Accelerator
- Aneutronic Fusion
- Magnetic Confinement
- Inertial Electrostatic Confinement
- Penning Trap
- Particle Accelerator
- Proton–proton chain reaction
- Triple-alpha process
- Carbon-nitrogen cycle
References
- ^ US patent 3,386,883 (1968-06-04) P.T. Farnsworth, Method and apparatus for producing nuclear-fusion reactions.
- ^ US4,826,646 (PDF version) (1989-05-02) Robert W. Bussard, Method and apparatus for controlling charged particles.
- ^ US4,233,537 (PDF version) (1980-11-11) Rudolf Limpaecher, Multicusp plasma containment apparatus.
- ^ Todd H. Rider (1994-04-15). "A general critique of inertial-electrostatic confinement fusion systems". https://dspace.mit.edu/handle/1721.1/29869.
- ^ Fundamental limitations on fusion systems not in equilibrium p161
- ^ Atzeni S., Meyer-ter-Vehn J (2004). "The Physics of Inertial Fusion: Beam Plasma Interaction, Hydrodynamics, Hot Dense Matter". http://fds.oup.com/www.oup.co.uk/pdf/0-19-856264-0.pdf#page=11.
- ^ S. Son , N.J. Fisch (2004-06-12). "Aneutronic fusion in a degenerate plasma". http://w3.pppl.gov/~fisch/fischpapers/2004/Son_PLA_04.pdf.
- ^ Ralph W. Moir (1997). "Direct Energy Conversion in Fusion Reactors". http://www.askmar.com/Fusion_files/Direct%20Energy%20Conversion%20in%20Fusion%20Reactors.pdf.
- ^ "Electricity Conversion by Neutralization Process" (Flash video). 2008-12-16. http://www.youtube.com/watch?v=YXLshYYsK8I.
- ^ "Spacecraft Propulsion" (Flash video). 2008-12-16. http://www.youtube.com/watch?v=oqHFowOge_M.
- ^ G. L. Kulcinski (2000-10-15). "Advanced Fusion Fuels Presentation". http://fti.neep.wisc.edu/presentations/glk_ans00.pdf.
- ^ E. N. Slyuta (2007). "The estimation of helium-3 probable reserves in lunar regolith". http://www.lpi.usra.edu/meetings/lpsc2007/pdf/2175.pdf.
- ^ Andrew Seltzman (2008-05-30). "Design Of An Actively Cooled Grid System To Improve Efficiency In Inertial Electrostatic Confinement Fusion Reactors". www.rtftechnologies.org. http://www.rtftechnologies.org/Design/Assets/device-images/fusor-mark3/files/seltzman_andrew_h_200805_phys.pdf. Retrieved 2009-08-14.
- ^ "Bremsstrahlung Radiation Losses in Polywell Systems", R.W. Bussard and K.E. King, EMC2, Technical Report EMC2-0891-04, July, 1991
- ^ James H. Underwood (2001-01-31). "X-Ray Data Booklet - Multilayers and Crystals". http://xdb.lbl.gov/Section4/Sec_4-1.pdf.
- ^ A.F. Jankowski, et al. (2004-10-22). "Boron–carbide barrier layers in scandium–silicon multilayers". http://www.me.ttu.edu/files/jankowski_me2311/tsf469470_scb4csi.pdf.
- ^ David L. Windt, et al. (2009-10-10). "Performance optimization of Si/Gd extreme ultraviolet multilayers". http://www.rxollc.com/windt/papers/2009_AppOp_48_5502.pdf.
- ^ "Nuclear Fusion Reactor - Calculations". http://www.crossfirefusion.com/nuclear-fusion-reactor/calculations.html. Retrieved 2009-12-15.
- ^ Dr. Tony Phillips, Science@NASA. "Honey, I Blew up the Tokamak". http://science.nasa.gov/headlines/y2009/31aug_mms.htm. Retrieved 2009-12-18.
- ^ E. N. Slyuta (2007). "The estimation of helium-3 probable reserves in lunar regolith". http://www.lpi.usra.edu/meetings/lpsc2007/pdf/2175.pdf.
- ^ S. Son , N.J. Fisch (2004-06-12). "Aneutronic fusion in a degenerate plasma". http://w3.pppl.gov/~fisch/fischpapers/2004/Son_PLA_04.pdf.
- ^ Ralph W. Moir (1997). "Direct Energy Conversion in Fusion Reactors". http://www.askmar.com/Fusion_files/Direct%20Energy%20Conversion%20in%20Fusion%20Reactors.pdf.



