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The energy emission taking place when orbital electron rings expand, can b=
e observed in the case when chemical explosives such as TNT (trinitrotoluen= ) explodes. The outermost orbital electron rings of their component atoms c= ontributing to combine them, expand only a little bit in this case of explo= sion, due to dissociation of TNT to form various kinds of gas molecules, su= ch as H2O, CO2, and NO2 etc. It is well known that the explosion of only about 7 kgs of uranium 235 pro= duces such an enormous energy equivalent to that emitted by explosion of TN= T 20,000 metric tons. The mass ratio of these two explosive materials is a= bout, 1 : 2.86x10^6. If the orbital electron rings in K shell of uranium at= om with radial parameter, say, =CE=B3=3D1/100, expands to be the orbital el= ectron rings in K shell of newly created atoms that has radial parameter, s= ay, =CE=B3=3D1/99.28, then the ratio of energy capacity of these two orbita= l electron rings becomes the same as the mass ratio, 2.86x10^6 , as shown a= bove when we estimate it with Eq.=E2=96=B3E=3DE'(1/r^4, previously posted. = The difference of radial parameter between these two electron rings is neg= ligibly small, or =CE=94=CE=B3=3D1/99.28-1/100=3D1/13,789, but the ratio of= their energy capacity is enormous, as shown above. However, this energy em= ission comes only from the expansion of orbital electron rings in K shell o= f uranium 235. Other orbital electron rings in L, M, N,. . . .shells of ura= nium 235 would also have to expand their orbital radii emitting huge energi= es also as in the case of electron rings of K shell. Thus the explosion of = only 7 kg of uranium 235 gives rise to producing such a tremendous energy. The fundamental mechanism of emitting energy from nuclear fusion of deuter= ons is exactly the same as that of nuclear fission of uranium 235. It is al= so the expanding energy of electron rings. In the case of nuclear fission a= tomic electron rings expand, while in the case of nuclear fusion nuclear e= lectron rings associated in the structure of two deuterons expand, emitting= nuclear energy. When nuclear electron rings of two deterons combine to bui= ld a unified nuclear electron ring with pair electrons, they have to expand= their orbital radii emitting energy, in order to bind four protons to buil= d two neutrons and two protons in a helium nucleus. This is the nuclear fus= ion energy. It is the same as that when two hydrogen atoms combine to form = a hydrogen molecule having molecular electron rings carrying pair electrons= , with their two single atomic electron rings, emitting energy. A single nuclear electron ring that binds two protons in constructing a ne= uteron, can emit =CE=B3-rays at the nearest distance to its two nuclear pro= tons when it breaks. Since this single nuclear electron ring can emit =CE= =B3-rays with wavelength 0.005 =E2=84=AB, its radial parameter must be, =CE= =B3=3D1/430, when we estimate it with the same equation, =E2=96=B3E=3DE'(1/= r^4) I posted above. If these single nuclear electron rings expand their or= bital radii and emit energy equivalent to that energy given by explosion of= 7 kgs of uranium 235, their radial parameter has to expand from =CE=B3=3D1= /430 to =CE=B3=3D1/429.991. The distinction between them is, =E2=96=B3=CE= =B3=3D1/429.991-1/430=3D1/20,544,014. It is an awfully small expansion comp= ared to that in the case of nuclear fission. However the energy emission in= the process of nuclear fusion is the same as that in the case of nuclear f= ission. The ratio of atomic volume of deuterium and helium is, D : He =3D 1= 4=2E1 : 31.8. The larger atomic volume of helium than deuterium is attribut= ed to the reason that the helium nucleus is stabilized in the lowest energy= level than deuteron. Nuclear fusion energy includes also the energy of orb= ital electron rings of deuterium when they expand their orbital radii to be= those of helium. newedana |
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