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Laser Optics & Photonics and Atomic & Plasma Science 2018
J u l y 1 6 - 1 7 , 2 0 1 8
P r a g u e , C z e c h R e p u b l i c
Page 70
American Journal of Computer Science and Information Technology
ISSN: 2349-3917
E u r o S c i C o n J o i n t E v e n t o n
Laser Optics & Photonics and
Atomic & Plasma Science
I
f the bunches of charged particles of same species (protons) are injected to a
point „F“, where two magnetic fields (perpendicular to each other) are applied
,the charged particles (the protons) of the first bunch will undergo to a confined
circular path and will pass through this point “F“ (point of injection ) by time
and again and thus the confined protons will be available for the protons of
the later injected bunch (reaching at point “F“) to be fused with at point “F“.
As the proton of later injected nth bunch reaches at point “F”, it fuses with the
proton of the first injected bunch (that has already confined) passing through
the point “F“. At point “F“, the two protons fuse and form a compound nucleus.
The compound nucleus splits and the deuteron (and the positron) is produced.
The produced deuteron, due to applied magnetic fields, undergo to a circular
orbit. The produced deuteron starts its circular motion from point “F“ (the point
of production of deuteron) and pass through this common tangential magnetic
field point “F” (or the point of production of nucleus) by time and again during
its circular motion .Thus the produced deuteron is confined and so the produced
deuteron will be available at point “F“ (the point of injection) for the proton of
later injected bunch (that is reaching at point “F“) to be fused with. Exhausting
the produced non – useful charged nuclei: The produced positron annihilates
with free electron and produces two gamma ray photons that in turn heat the
tokamak. As the proton of later injected bunch reaches at point “F“, it fuses with
the confined deuteron (passing through the point “F“) and form the helium -3
nucleus. The produced helium -3 nucleus starts its circular motion from point
“F“ (0,0,0) or the point p1(x1 , y1, z1) and reaches at point p2 (x2 , y2 , z2) located
on the circumference of the circle to be followed by the helium -3 nucleus. As
the helium -3 nucleus reaches at point p2 (x2, y2 , z2), it enters into the mouth
of the horse pipe that is located at the point p2 (x2 y2 z2) and thus the helium -3
nucleus is extracted out of the tokamak with the help of vacuum pump attached
to the another end of horse pipe. Thus we can establish a steady state controlled
nuclear fusion reactor based on H-H cycle.
VBM fusion reactor H – H cycle
Badri Lal Manmya
1
VBM Fusion Reactor, India
Badri Lal Manmya, J Food Nutr Popul Health 2018, Volume: 2
DOI: 10.21767/2577-0586-C1-003
Biography
Badri Lal Manmya completed his education in JNV Hurda (
Rajasthan) and completed his Diploma also got Teacher's
training certificate and now working as a Teacher in state
government of Rajasthan. His Research interest- plasma
physics,to establish a steady state controlled nuclear fusion
reactor based on hydrogen cycle and also based on D - D cycle.
Books written by him are VBM fusion reactor H - H cycle and
VBM fusion reactor D - D cycle.
badrilalmanmya@gmail.com