|
Taxon 5.4
BLACKSTELLIDES
| Semistable objects that peakmassed between 25 and 45 solarmasses. |
|
|
Work in progress
| Taxon 5.4 - BLACKSTELLIDES |
|
Work in progress
| Taxonome 5.4.1 - BLACKSTARS |
Blackstars
- Blackstars are understable blackstellides.
- Blackstar primary content is nucleons and nuclides.
- Blackstars are a nucleus, substrate, atmosphere, teelosphere, gravitysheath and gravitysheath interface.
- Blackstars peakmass between 25 and 45 solarmasses.
- Blackstar undergo nucleon and nuclide collapse during semistabilisation.
- Blackstar collapses are gravitycollapse, emissioncollapse, fusioncollapse, ferriccollapse, and fissioncollapse.
Caveat
The factbase for blackstar interiors is sparse. Thus blackstar naxosnumbers are mostly high. Thus this description
taxonomically is unsound.
Caveat The fate of most blackstars is to be accreted into something larger before they can semistabilise as blackstellides.
Mechanics
- Blackstar nuclides stratify by isotopenumber as conditions permit.
- Nuclide stratification is lowest isotopenumber outmost to highest isotopenumber inmost as conditions permit.
- Blackstars stratify by nuclide bonds as conditions permit.
- Blackstar stratification is gasbonding outmost through liquidbonding to solidbonding inmost.
- Blackstars semistabilise as blackstellides.
- Semistabilisation is achieved by ejecting more gravitymassvelocity than is absorbed.
- Gravitymassvelocity ejections
result in gravitycollapse, emissioncollapse, fusioncollapse,
ferriccollapse, and fissioncollapse.
- Gravitycollapse is blackstar contraction by teel ejections.
- Emissioncollapse is proton / nuclide contraction by photon emissions.
- Fusioncollapse is nuclide stratum contraction by nuclide fusions.
- Ferriccollapse is nucleus contraction by nuclide fusions.
- Fissioncollapse (1) is compression of inner nucleus by nuclide fission.
- Fissioncollapse (2) is expulsion of outer nucleus / atmosphere by nuclide fission.
Nucleus
- Blackstar nucleuses are the core of a blackstar.
- Such nucleuses are inside an atmosphere.
- Such nucleuses are solidbonded and/or liquidbonded as conditions permit.
- Such nucleuses (1) are an inner nucleus of blackferric nuclides.
- Such nucleuses (2) are an outer nucleus of whiteferric nuclides.
- Nuclides stratify by isotopenumber as conditions permit.
- Nuclide stratification is lowest isotopenumber outmost to highest isotopenumber inmost.
- Highest isotopenumber equates to blackstar peakmass.
- Nucleus whiteferric fusions result in ferriccollapse.
- Ferriccollapse results in nucleus contraction.
- Nucleus blackferric fissions result in fissioncollapse.
- Fissioncollapse results in inner nucleus compression.
Substrate
- Substrate primary content is fundamides, photides, and morphides.
- Such content is emitted / ejected by nucleons / nuclides.
- Substrate secondary content is stripped neutrons and stripped primalnuclides.
- Secondary content is drawn down from the atmosphere by blackstar intrinsic gravitypull.
- Substrate content moves in between nuclides.
- Such substrates (1) move through nuclide teelospheres.
- Such substrates (2) are carried by teelstream systems.
- Substrate heft increases as ejections / emissions into it increase.
- Such increases decrease nucleon / nuclide packingdensity.
- Substrate heft decreases with content absorption into nucleons / nuclides.
- Such absorptions reinforce nucleon / nuclide engorgement.
- Decreases in substrate heft increase potential nucleon / nuclide packingdensity.
- Potential packingdensity is made extant (1) by mutual gravitypull of nucleons / nuclides.
- Potential packingdensity is made extant (2) by blackstar intrinsic gravitypull.
- Packingdensity increases are blackstar collapse.
- Before blackstar peakmass is achieved substrate heft dominates blackstar collapse.
- After blackstar peakmass is achieved (1) blackstar collapse dominates substrate heft.
- After blackstar peakmass is achieved (2) substrate is increasingly squeezed toward blackstar surface.
Caveat:
Teelstream systems move between blackstar surface and
blackstar centre. Teelstream heft increases from surface to centre as
potential transmutes to extant. As heft increases substrate objects
must be more gravitymassive to attune before overengorgement and dissipation. Especially with monocore
objects. Within the nucleus (1) it may or may not be that all
monocore objects are dissipated into the now very hefty
teelstreams. Within the nucleus (2) it may or may not be that the substrate content is only stripped neutrons and heliums.
- Atmosphere primary content is gasbonded nucleons and nuclides.
- Secondary content is stripped neutrons and stripped primalnuclides.
- Secondary content forms in the outer atmosphere and is drawn to the inner atmosphere blackstar intrinsic gravitypull.
- Nuclides stratify by isotopenumber as conditions permit.
- Nuclide stratification is lowest isotopenumber outmost to highest isotopenumber inmost.
- Atmospheres are stratified by mechanisms.
- Atmosphere stratification is photosphere outmost through neutronosphere and primasphere to lithisphere inmost.
- Photosphere primary content is engorged protons.
- Photosphere primary mechanism is emissioncollapse.
- Neutronosphere primary content is engorged neutrons.
- Neutronospheres circulate engorged neutrons to the photosphere and stripped neutrons to the primasphere.
- Primasphere primary content is primalnuclides.
- Primasphere primary mechanism is manufacture of nucleons, heliums, and lithiums.
- Lithisphere primary content is lithicnuclides.
- Lithisphere primary mechanism is fusioncollapse.
Teelosphere
- Blackstar teelospheres are a teelstream system.
- Blackstar teelstream systems are a complex of subsidiary systems.
- Blackstar teelstream systems course throughout.
- Blackstar teelstream systems are primarily driven by blackstar spin.
- Teelstream systems are axial, centrifugal, chaotic, or a mix.
- Teelstream systems are local or global.
- Local systems are confined to a stratum or region.
- Global systems move between blackstar centre and gravitysheath interface.
- Global systems eject excess teels across the gravitysheath interface.
- Teel ejection is blackstar gravitycollapse.
- Teelstreams engorge morphides / nuclides.
- Teelstreams cationise axial morphides / nuclides.
- Teelstreams carry substrate.
- Teelstreams carrying morphides / nuclides are a plasmastream.
Gravitysheath
- Blackstar nucleuses are surrounded by a gravitysheath.
- Gravitysheaths are surrounded by a gravitysheath interface.
- Gravitysheath
interfaces enclose a region within which the gravitypull of the nucleus
is stronger than the gravitypull of any other object.
- Gravitysheath interfaces abut the gravitysheaths of adjacent objects.
- Adjacent objects with a gravitysheath wholly inside the gravitysheath interface of a blackstar are dominance adjacent.
Fusion
- Fusion (1) is strongforcing nucleon to nucleon to make primalnuclides.
- Fusion (2) is strongforcing cationed nuclide to stripped object to make heavier nuclide isotopes.
- Primalnuclide / lithicnuclide fusions are common to all types of star.
- For details of such fusions: cf: dwarfstar.
- Whiteferric nuclide fusions are common to whitestars, blackstars, and galastars.
- For details of such fusions: cf: whitestar.
- Blackferric nuclide fusions are common to blackstars and galastars.
- Primalnuclide / lithicnuclide fusions take place in blackstar atmospheres.
- Primalnuclides are elementnumbers 1 and 2.
- Blackstar primalnuclides are engorged.
- Lithicnuclides are elementnumbers 3 to 25.
- Blackstar lithicnuclides are engorged.
- Atmosphere fusions eject more gravitymassvelocity than is absorbed.
- Such fusions reduce ejection quantity with each heavier isotopenumber.
- Pre blackstar peakmass - such fusions maintain or expand the atmosphere volume.
- Post blackstar peakmass - such fusions do not maintain or expand atmosphere volume.
- Whiteferric nuclide fusions take place in blackstar outer nucleuses.
- Whiteferrics are elementnumbers 26 to 82.
- Blackstar whiteferrics are (1) engorged.
- Blackstar whiteferrics are (2) overstable.
- Whiteferric fusions absorb more gravitymassvelocity than is ejected.
- Such fusions decrease ejection quantity with each increase in isotopenumber.
- Such fusions contract outer nucleus volume.
- Blackferric nuclide fusions take place in blackstar inner nucleuses.
- Blackferrics are elementnumbers 83 to 118.
- Blackferrics may fuse to elementnumbers higher than 118.
- Blackstar blackferrics are (1) engorged.
- Blackstar blackferrics are (2) overstable.
- Blackferric fusions absorb more gravitymassvelocity than is ejected.
- Such fusions decrease ejection quantity with each increase in isotopenumber.
- Such fusions contract inner nucleus volume.
Fission
- Fission is splitting an understable isotope into lesser isotopes.
- Fission results in fundamide and/or photide and/or morphide ejections.
- Fission takes place in blackferric isotopes.
- Fission ability is not in all blackferric isotopes.
- Fission is spontaneous or induced.
- Spontaneous fission is random in time and conditions.
- Random fissioning may or may not result from structural flaws.
- Up to 50 spontaneous fissioning isotopes are known.
- Spontaneous fissioning degree varies from type to type.
- Notable spontaneous fissioning isotopes are Uranium-238 and Plutonium-240.
- Induced fission results from isotopes absorbing energetic objects.
- Such absorptions increase isotopenumber.
- Such absorptions are commonly of stripped objects.
- Induced fission may or may not result from structural flaws.
- Such fission is possible in many heavy isotope types.
- Induced fission ability degree varies with isotope type.
- Notable induced fissioning isotopes are Uranium-233, Uranium-235, and Plutonium-239.
Fissioncollapse
- Fissioncollapse is triggered by chainreaction fissiondecay in stratums of blackferric isotopes.
- Chainreaction fissiondecay begins with the fissioning of isotopes capable of spontaneous fissiondecay.
- Chainreaction fissiondecay continues with the fissioning of isotopes capable of induced fissiondecay.
- As conditions permit blackferric isotopes stratify by isotopenumber.
- Stratums form (1) of isotopes capable of spontaneous fission.
- Stratums form (2) of isotopes capable of induced fission.
- Such stratums become criticalmasses when sufficiently gravitymassive.
- Spontaneously fissioning isotopes eject energetic neutrons / heliums.
- Neutrons / heliums are absorbed by fission capable isotopes.
- Such isotopes fission.
- Fissioning isotopes eject further energetic neutrons / heliums.
- Chainreactions of absorptions / ejections begin.
- Such chainreactions fission whole stratums.
- Such chainreactions fission adjacent stratums.
- Stratum fissions are both explosion and implosion.
- Stratum explosion ejects stratums outside the fissioning stratums.
- Some or all ejections cross the gravitysheath interface of the remaining blackferric core.
- Stratum implosion compresses stratums inside the fissioning stratums.
- Such inside stratums are collapsed.
- Such collapse may or may not be to a solidbonded teelcore.
- Such a core is a rapidly spinning sphere.
- Sphere gravitypull results in surrounding eventhorizon.
- The sphere is a blackhole.
Aftermath
- Blackholes are initially understable.
- Blackholes of 2 to 4 solarmasses are possible.
- Blackholes of multi-million solarmasses are at galastar centres.
- Blackholes semistabilise as blackstellides.
- Semistabilisation is primarily by gravitycollapse.
- Such gravitycollapse is teel ejection.
- Accretion continues if accretables are available.
- Sufficient accretion reactivates a blackstellide as a blackstar.
- Sufficient further accretion evolves a blackstar into a galastar.
|
© 2024 - Ed Winchester / Sian Winchester
|
|
SUPERSEDED MATTER
BLACKFERRIC A ferricnuclide element that has no stable isotopes.
WHITEFERRIC A ferricnuclide element that has at least one stable isotope.
[] INDUCED FISSIONDECAY A decay mechanism in understable blackferric isotopes during blackstar fissioncollapse.
[] SPONTANEOUS FISSIONDECAY A decay mechanism in understable blackferric isotopes.
FUSION
Strongforcing nucleons and/or nuclides together to create a more gravitymassive nuclide.
FISSIONCOLLAPSE
A semistabilisation mechanism in
blackstars that contributes to semistabilising a blackstar by fissioning its
stratums of blackferric isotopes and ejecting some or all of its stratums of primalnuclides, lithicnuclides, and white ferricnuclides.
BLACKHOLE An object with a massdensity so high it is always inside a darksphere.
There are two forms of blackhole: stellar blackholes and galactic blackholes.
- Stellar blackholes These result from the collapse of hypergiantstars.
- Galactic
blackholes These form inside the darkspheres that form
around the gravitycentres of galaxies with enough mass.
* * * * *
Hypergiantstars
have enough mass to fuse stratums of transuranic isotopes inside
stratums of fissile isotopes. When the fissile stratums reach
critical mass they implode. The transuranic stratums are simultaneously
overengorged and crushed together. The transuranic isotopes are broken
into lesser isotopes. Much of the isotope teelospheres are expelled out
to reinforce the fission explosion.
What remains is a compact
sphere of stripped isotopes surrounding a core of stripped nucleons.
The exact mix depends on the peakmass of the hypergiantstar. The higher
the peakmass the higher the proportion of nucleons over isotopes. It is
possible that the higher peakmass hypergiantstars collapse to have a
central core of solidbonded teels. It may even be possible that the
highest peakmass hypergiantstars collapse to an object that is entirely
solidbonded teels.
It
is possible that hypergiantstars pre collapse already have a darksphere
surrounding their gravitycentre. Certainly, the post collapse
blackhole has one surrounding its gravitycentre. At their least
massive, the surface of the darksphere and the surface of the
blackhole coincide. With increases in blackhole mass, the volume
of the darksphere increases more than does the volume of the
blacksphere.
Stellar blackholes are not inert. Notably,
they have teelospheres formed into substantial and active
teelstream systems. The systems extend beyond the darkspheres.
The
extrinsic gravitypull of stellar blackholes is such that they
accrete anything that comes within range that is not so big that it
will accrete them. That said, most of the feedstock of any blackhole is
subphotonic. The subphotonic mass of many galaxies is believed to be
upwards over 70% of the total mass so there is plenty of that feedstock
available.
The act of accretion makes a blackhole understable or
more understable. Thereafter they undergo stabilisation by ejecting
teels. A blackhole that is continually accreting and thus in continuous
stabilisation is a blackhole that is increasing its mass. A
stable blackhole is a cold blackhole, one which is neither accreting
nor ejection. Whether there are yet any cold blackholes in the Universe
is unknown.
* * * * *
Galaxies are accumulations of stars bound together by their mutual gravitypull. At their centre galaxies have
- Masscentre The point around which the stars move and to which they are ultimately attracted.
- Gravitycentre.
Where the intrinsic gravitypull of the
galaxy cancels out. The gravitycentre can be a point and
the cancellation total. However, more likely it is a sphere
and the cancellation to a degree.
If
a galaxy has enough mass, the gravitycentre becomes a
darksheath, a region from within which an object can only escape
if it can exceed the escapevelocity at the darksheath surface. Galaxy
mass increases commensurately increase the darksheath volume and the
darksheath surface escapevelocity. A sufficient increase raises the
surface escapevelocity to lightspeed.
- Objects in a darksheath decelerate moving toward the gravitycentre.
- Objects in a darksheath accelerate moving away from the gravitycentre.
- Objects with a sufficiently low entry speed can be held in trojan adjacency.
- Objects that lose speed in collisions can be held in trojan adjacency.
- Trojan objects aggregate, begin to spin, and have an extrinsic gravitypull.
- The trojan aggregate is now the blackhole at the centre of the darksheath.
- The blackhole extrinsic gravitypull actively accretes objects into the darksheath.
- Accreted objects are dissipated and absorbed into the blackhole.
- The mass of the blackhole grows.
- At
the surface of the darksheath, a massvelocity of zero relative to the
masscentre supplants the escapevelocity of lightspeed relative to
the gravitycentre.
The
primary "feedstock" of blackholes is subphotonics (darkmatter). The
above description reflects this. However, process is accelerated
if one or more stars becomes trojan adjacent at an early
stage.
Blackholes of sufficient mass have a substantial
high-momentum teelocean. Objects drawn into the teelocean are broken
down and assimilated.
Blackholes have teelospheres formed
into high-momentum teelstream systems. As the mass of blackholes
increase, the teelospheres extend further and further out into the
gravitysheath. The very dense inner break down more that extend
beyond the darksheath. These break down more substantial objects by
overengorgement and gravitational spaghettification.
Accretion
understabilises a blackhole, triggering stabilisation by ejection,
emission, and expulsion. However, as the mass of the blackhole
increases it can first no longer expel and then no longer emit.
However, understable blackholes all eject. The surrounding teelstream
systems are the means by which blackholes eject their excess
massvelocity and energyvelocity out of their gravitysheaths.
Per
the energy/mass differential, understable blackholes are increasing
their measures of energy and mass. Blackholes only stop growing when
there is nothing to be accreted. By default, understable blackholes
increase and its escape velocity rises, it firstly can no longer
expel and then, as the escapevelocity exceeds lightspeed, it can no
longer emit. From hereon stabilisation is by the ejection of teels.
The
energy/mass differential means that as long as the blackhole can keep
on accreting it can keep on growing. , then it cannot emit,
The extrinsic gravitypull of galactic |
DARKSHEATH A region enclosed by a surface at which the escapevelocity is a smidgeon above lightspeed.
Photons
only move at lightspeed. Thus a photon inside a
darksheath can never accelerate enough to escape.
Superphotonics are unable to move as fast as lightspeed and thus
cannot escape either. Subphotonics, however, can and do exceed
lightspeed. Thus subphotonics can and do escape from darksheaths.
There are two forms of darksheath: stellar darksheaths and galactic darksheaths.- Stellar dark spheres These surround the blackholes that result from the collapse of hypergiantstars.
- Galactic
dark spheres These form around the gravitycentres of
galaxies with enough mass. Thereafter, blackholes can form
inside the darksheaths from incoming accretions.
CAVEAT
The Current Paradigm, largely due to the dominance of
some logictraps and quasifacts, does not seriously differentiate
between the event horizon of a blackhole and the blackhole itself.
hypothesize
. it has a degree of knowledge of the behavior of , albeit
circumstantial evidence, that might A darksheath is a part of
that The Current Paradigm does not seriously differentiate between the
event horizon of a blackhole and
The collapse of a hypergiantstar
results in a contracted object of high mass and small volume, the
extrinsic gravitypull of which is sufficient to erect a darksheath. The
greater the mass of the contracted object, the greater the volume of
its darksheath.The
darksheath inside a galactide is initially a consequence of the mutual
gravitypull of its stars. If the galactides intrinsic gravitypull is
sufficient, a darksheath forms around the masscentre. In principle,
there need be no matter at all inside the darksheath. However, since
photons and superphotonics will enter and be unable to leave, the
darksheath soon acquires mass of its own and its volume expands
accordingly.
THINK ON THIS FOR THE BLACKHOLE ENTRY
The
combined mutual gravitypull of the stars in a galactide is the
galactide's intrinsic gravitypull. The locus of the intrinsic
gravitypull is the galactide's masscentre - the point around which
galactide's stars move and to which they are ultimately attracted.
However, the masscentre is also the galactide's gravitycentre - the
point at which the gravitypulls of the galactide's stars is equal and
opposite. Initially there need not be anything at the gravitycentre but
if the galactide is massive enough something will soon be held there in
trojan adjacency. What is held doesn't need to be substantial. A teel
or a subphotonic is enough to give the "gravitycentre" an extrinsic
gravitypull of its own.
s
also a gravitycentre. results in a gravitycentre . There need not
initially be anything at the gravitycentre darksheath inside a
galactide is initially a
consequence of the mutual gravitypull of its stars. If the galactides
intrinsic gravitypull is sufficient, a darksheath forms around the
masscentre. In principle, there need be no matter at all inside the
darksheath. However, since photons and superphotonics will enter and be
unable to leave, the darksheath soon acquires mass of its own and its
volume expands accordingly.
CAVEAT
In the Current Paradigm, the term event horizon roughly
equates to darksheath and blackhole equates to the massive object
within. However, neither term is exactly accurate and both
have implications and connotations that do not sit well with Core
Physics.
While extrapolations out of Core Physics can broadly
suggest the likely form of the massive object inside a
darksheath, more facts are needed before a useful description can be
compiled. In the meantime, darksheath is used as a coverall for both
event horizon and black hole. The word may not be as much fun but it is grammatically correct and scientifically true.
As an aside, darksheath sits well with darkenergy and darkmatter as entities that interact but cannot be seen. |
S3 STARS- Peakmass between 25 and 40 or more solarmasses.
STRUCTURELIFECYCLE- S3 stars -
- S3 stars
- S3 stars -
- Sequentially then simultaneously, undergo -
- Ferriccore contraction.
- Chainreaction contraction.
- Stabilisation as S quark.
STABILISATIONPLASMATISATION- S3 star interiors are circulating plasmastreams.
- S3 star isotopes are stratified inwardly by increasing massdensity.
- Plasmastream circulations are vertical, horizontal, and often vortexed.
- Plasmastreams cross the interfaces between isotope stratums.
- Isotopes move with plasmastreams but their ability to move out of their stratums is limited.
- Plasmastream circulation patterns are influenced but not dominated by the isotopes within them.
- Isotope circulation patterns are influenced but not dominated by the plasmastreams they are within.
CONTRACTION- S3 stars -
- Contraction rates increase with peakmass.
- Contraction reduces space between isotope nuclei.
- Some /all subferric stratums expelled from star.
- Subferric stratums expelled increases with peakmass.
COLLAPSE- S3 stars -
- Fuse core of fissionable isotopes inside subfissile isotope stratums.
- Fuse core of fissile radioisotope stratums fissionable isotope stratums.
- Transuranic stratums compressed to teelcore.
- Subfissile stratums expelled from star.
- Collapse dominates when stars undergoing contraction /collapse simultaneously.
ACCRETIDES A taxa of three taxons: protostars, contractastars, and collapsastars.
COLLAPSASTARS Objects that grow by accretion to have a peakmass high enough for fission.
COLLAPSASTAR STRUCTURE
COLLAPSASTAR LIFECYCLECOLLAPSASTAR STABILISATION
COLLAPSASTAR PLASMATISATION
- Collapsastar interiors are circulating plasmastreams.
- Collapsastar isotopes are stratified inwardly by increasing massdensity.
- Plasmastream circulations are vertical, horizontal, and often vortexed.
- Plasmastreams cross the interfaces between isotope stratums.
- Isotopes move with plasmastreams but their ability to move out of their stratums is limited.
- Plasmastream circulation patterns are influenced but not dominated by the isotopes within them.
- Isotope circulation patterns are influenced but not dominated by the plasmastreams they are within.
COLLAPSASTAR CONTRACTION
COLLAPSASTAR COLLAPSE
CAVEAT BLACKHOLES
Hypergiantstars
have enough mass to fuse stratums of transuranic isotopes inside
stratums of fissile isotopes. When the fissile stratums reach
critical mass they implode. The transuranic stratums are simultaneously
overengorged and crushed together. The transuranic isotopes are broken
into lesser isotopes. Much of the isotope teelospheres are expelled out
to reinforce the fission explosion.
What remains is a compact
sphere of stripped isotopes surrounding a core of stripped nucleons.
The exact mix depends on the peakmass of the hypergiantstar. The higher
the peakmass the higher the proportion of nucleons over isotopes. It is
possible that the higher peakmass hypergiantstars collapse to have a
central core of solidbonded teels. It may even be possible that the
highest peakmass hypergiantstars collapse to an object that is entirely
solidbonded teels.
It
is possible that hypergiantstars pre-collapse already have a darksheath
surrounding their gravitycentre. Certainly, the post-collapse
blackhole has one surrounding its gravitycentre. At their least
massive, the surface of the darksheath and the surface of the
blackhole coincide. With increases in blackhole mass, the volume
of the darksheath increases more than does the volume of the
blacksphere.
Stellar blackholes are not inert. Notably,
they have teelospheres formed into substantial and active
teelstream systems. The systems extend beyond the darksheaths.
The
extrinsic gravitypull of stellar blackholes is such that they
accrete anything that comes within range that is not so big that it
will accrete them. That said, most of the feedstock of any blackhole is
subphotonic. The subphotonic mass of many galaxies is believed to be
upwards over 70% of the total mass so there is plenty of that feedstock
available.
The act of accretion makes a blackhole understable or
more understable. Thereafter they undergo stabilisation by ejecting
teels. A blackhole that is continually accreting and thus in continuous
stabilisation is a blackhole that is increasing its mass. A
stable blackhole is a cold blackhole, one which is neither accreting
nor ejection. Whether there are yet any cold blackholes in the Universe
is unknown.
|
Objects resulting from the collapse of hypergiantstars.
|
VERSION 26TH MAY 2021
STRIPPED DEUTERIUMS Engorged deuteriums with reduced gravitysheaths and commensurately reduced teelospheres and repellence.
STRIPPED HELIUMS Engorged heliums with reduced gravitysheaths and commensurately reduced teelospheres and repellence.
Helium stripping happens in plasmastreams when an engorged helium isotope enters the gravitysheath of an engorged more massive isotope (dominance adjacency). There is a consequent reduction in the volume of the helium's gravitysheath. The closer the helium is to the nucleus of the dominant isotope, the greater is the reduction. The greater the mass of the dominant isotope, the greater is the reduction.
- A Helium-4 nucleus is symmetrical and tightly bound.
- A Helium-4 teelosphere is centrifugal.
- A helium's engorged teelosphere fills the gravitysheath.
- A heliums gravitysheath volume is reduced inside the gravitysheath of a dominant isotope.
- Reducing the gravitysheath volume reduces the teelosphere volume.
- Reducing the teelosphere volume ejects teels into the teelosphere of the dominant isotope.
- Ejecting teels reduces the helium's teelospheric repellence.
- Reductions in teelospheric repellence increase with increasing closeness to the dominant nucleus.
- Reductions in teelospheric repellence increase with increases in the mass of the dominant nucleus.
- A
sufficiently massive dominant isotope will strip a sufficiently close
helium of all teelosphere and thus of all teelospheric repellence.
- The repellence of a wholly stripped helium is that of its nucleus only.
Stripping the teelospheric repellence from a helium is a significant factor in the fusion process. A reduction in repellence is a reduction in resistance to the gravitypull of a dominant isotope. Strip away enough resistance and a helium can collide with its dominant nucleus. If the collision is at the right speed, the right inclination, and at a sweet spot, the two nuclei strongforce together. Once the consequent ejections, emissions, evictions, and transmutations are complete, they have fused into a more massive isotope.
The structure of a Helium-4 nucleus is tightly bound and with a substantially higher massdensity than all more massive isotopes. Consequently heliums mostly maintain their identity when fusing. Thus Carbon-12 is three Helium-4, Oxygen-16 is four Helium-4, and so on.
Stripped of much of the teelospheric repellence, heliums move with relative ease between (and colliding but not fusing with) dominant isotope nuclei. They can travel substantial distances with the direction of that travel being, overall, downward. Having a greater massdensity than any dominant isotope, they respond to the intrinsic gravitypull of their star and move toward the masscentre.
|
STRIPPED NEUTRONS Engorged neutrons with reduced gravitysheaths and commensurately reduced teelospheres and repellence.
Neutron stripping happens in plasmastreams when an engorged neutron enters the gravitysheath of an engorged isotope. There is a consequent reduction in the volume of the neutron's gravitysheath. The closer the neutron is to the nucleus of the isotope, the greater is the reduction. The greater the mass of the isotope, the greater is the reduction.
- A neutron teelosphere is centrifugal.
- An engorged centrifugal teelosphere fills the neutron gravitysheath.
- The volume of a neutron gravitysheath, when inside an isotope gravitysheath, is reduced.
- Reducing the gravitysheath volume reduces the teelosphere volume.
- Reducing the teelosphere volume ejects teelmass into the isotope teelosphere.
- Ejecting teelmass reduces teelospheric repellence.
- Reductions in teelospheric repellence increase with closeness to the isotope nucleus.
- Reductions in teelospheric repellence increase with the mass of the isotope nucleus.
- An
isotope of sufficient mass will strip a neutron that is sufficiently
close of all its teelosphere and thus of all its teelospheric
repellence.
- The repellence of a wholly stripped neutron is that of its nucleus only.
Stripping the teelospheric repellence from a neutron is a significant factor in the fusion process. A reduction in repellence is a reduction in resistance to isotope gravitypull. Strip away enough resistance and a neutron nucleus can collide with an isotope nucleus. If the collision is at the right speed, the right inclination, and at a sweet spot, the two nuclei strongforce together. Once the consequent ejections, emissions, evictions, and transmutations are complete, they have fused into a more massive isotope.
Stripped of their teelospheric repellence, neutrons move with relative ease between (and sometimes colliding but not fusing with) isotope nuclei. They can travel substantial distances with the direction being, overall, downward. Having a greater massdensity than any isotope, they respond to the intrinsic gravitypull of their star and move toward the masscentre.
The ability of stripped neutrons to pass between isotope nuclei is crucial in the evolution of ferric isotopes. These consist of fifty or more nucleons most of which are as heliums. Stripped neutrons pass between the heliums to lodge at the masscentre of the isotope where they become a neutroncore, courtesy of their greater massdensity. The more massive the ferric isotope, the more neutrons are contained in its neutroncore.
Debatably, even before the contraction of contractastars or the collapse of collapsastars, stripped neutrons may, courtesy of their greater massdensity, form a plasmatised core at their masscentres.
|
|
|
|