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Taxa
GALACTIDES
TAXA Galactides Objects with blackstars in their nuclei.
TAXON Elliptogalaxies Galactides with a one blackstar, standard, nucleus.
TAXON Electrogalaxies Galactides with a two blackstar, electroidal, nucleus.
TAXON Nucleogalaxies Galactides with a three blackstar, nucleonic, nucleus. |
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BROUGHT FORWARD
GALACTIDES A taxa.
This is a holding entry
Galactides is a taxa consisting of taxons with a peakmass high enough to maintain a holisphere. The taxa has three taxons:
- Globulars Galaxies in dominance adjacency to larger galaxies.
- Galaxies Galaxies in type adjacency to other galaxies.
- Galactars Clusters of type adjacent galaxies bound by their mutual gravitypull.
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GLOBULAR A taxon.
GALAXIES A taxon.
GALAXIES A taxon in the taxa Galactides. Galaxies are galactides in type adjacency.
GALACTIDES A taxa consisting of taxons that grow by accretion and maintain a holisphere until dissipation or stabilisation. The taxa has three taxons: globulars, galaxies, and galactars.
GALAXY FACTBASE
The galaxy factbase is not extensive. It is limited by observing
distances and equipment inadequacy. Factbase expansions and
revisions are expected.
- A galaxy is a holisphere around a masscentre.
- Galaxies are in type adjacency to adjacent galaxies.
- Galaxies with enough mass are a nucleus of tightly bound stars and a halo of diffuse stars.
- Stars can be solo or in globulars.
- Galaxies vary widely in mass and, commensurately, in the number of stars they contain.
- Dwarf galaxies
Galaxies without enough mass to form a spiral disk of stars in
the halo. Such a galaxy, subject to circumstance, can be a type adjacent dwarf galaxy or a dominance adjacent globular. It may be that all dwarfs unable to accrete enough mass to become spirals are doomed to become globulars eventually.
- Spiral galaxies Galaxies with enough mass to form a spiral disk of stars in the halo. Spirals are common in the outer reaches of galactars and less common toward the centre.
- Elliptical galaxies Galaxies with enough mass to become a spheroid of of stars. Nuclei cannot
be seen. Disks (if any) cannot be seen. Elliptical galaxies are common
toward the centre of galactars and less common in the outer reaches.
- Galaxies with enough mass have a darksphere.
GALAXIES IN CORE PHYSICS Nothing in the galaxy factbase clashes with Core Physics expectations. These extrapolations from the Core Physics Taxonomic Table may provide insight.
- A star in a galaxy has its own gravitysheath.
- A star in a galaxy is in dominance adjacency.
- A globular in a galaxy has its own gravitysheath.
- A globular in a galaxy is in dominance adjacency.
- A galaxy observed by photon emission was understable at the time of emission.
- A galaxy unobservable by photon emission may, or may not, be understable.
- A galaxy with enough mass has a galactic darksphere.
- A galaxy with enough mass has a galactic darksphere with a galactic blackhole inside.
- A galactic blackhole in an understable galaxy is itself understable.
- Understable galactic blackholes stabilise per the energy/mass differential.
- Understable galactic blackholes stabilise by ejecting teels.
- Understable galactic blackholes cannot stabilise before its nucleus and halo.
- A galaxy has a teelstream system.
- Galaxy teelstreams may contain plasmatoids and be plasmastreams.
- Galaxy teelstreams have significant momentum in the nucleus.
- Teelstream momentum in the nucleus engorges the nucleus stars.
- Engorged star photospheres emit photons prodigiously.
- Engorgement in nucleus stars is reinforced by photon emission pressure.
- Engorgement inhibits all but the simplest fusions in nucleus stars.
- Engorgement in stars near, or inside, the darksphere is such that all fusion is inhibited.
- Photon emission from stars near, or inside, the darksphere is from understable protons in the photosphere and is intense.
- Galactic blackholes with enough mass overengorge stars near, or inside, the darksphere, dissipating and then accreting them.
- Halo stars undergo the fusion cycle commensurate with their peakmass and subject to the degree of their engorgement.
- Halo star "nurseries" accelerate the fusion cycle in stars by seeding each other with pre-fused isotopes.
- Over time, halo stars move toward the nucleus.
- Over time, nucleus stars move toward the darksphere and the blackhole.
- Over time, the galactic blackhole accretes all it can before stabilising as a cold blackhole.
CAVEAT Concern is being expressed by some researchers that the mass of some galactic blackholes is such that it cannot have been accreted inside the currently estimated time elapsed since the beginning of the Universe.@@@@@
- Time elapsed The age of the Universe needs to be reconsidered in the light of the Core Physics Taxonomic Table.
- Accretion rate
The Current Paradigm (with suspicion) recognises the existence
of darkmatter. It does not recognise it, however, as a significant
percentage of the "feedstock" of galactic blackholes. In Core
Physics, galactic blackholes do eat their own stars but they first
dissipate them into digestibles. Thus the feedstock is morphides,
photides, and fundamides. Yet much of the feedstock is
not dissipation material at all. It is photides and fundamides:
that is, photons and darkmatter. Given
that darkmatter in some galaxies is estimated to be over 80%
of the matter content, there is a lot of it there to be eaten.
CAVEAT
In the Current Paradigm, the metal-rare condition of stars in
galactic nuclei is taken as meaning the stars are old. They can be old,
of course, but the cause of their metal-rarity is because they are
engorged. Indeed, when galaxies have very massive galactic
blackholes, their lifespan can be short through being overengorged
and dissipated.
CAVEAT
The endpoint in the lifecycle of a galaxy is being accreted
or becoming stable - stable being without any ejections,
emissions, or expulsions. It may be that no galaxies in the
visible universe have yet stabilised.
CAVEAT
Galaxies are observed in a wide range of sizes and masses.
However, there is a size/mass beyond which no galaxies are observed.
Whether this is a limitation of some kind is currently unknown.
However, Core Physics currently suggests no reason for such a
limitation.
CAVEAT The
nucleus of a galaxy consists of strongforced stars engorged inside an
energetic teelstream system. The teelstream system inhibits the ability
of the stars to fuse the more massive isotopes. If the eventhorizon is
sufficiently massive, a limited number of stars are subforced to its
surface. |
GALACTARS A taxon.
GALACTIDES A taxa consisting of taxons with a peakmass high enough to maintain a holisphere. The taxa has three taxons: globulars, galaxies, and galactars.
GALACTARS Clusters of type adjacent galaxies bound by mutual gravitypull.
GALACTAR FACTBASE
The galactar factbase is thin. It is limited by great
observing distances and equipment inadequacy. Factbase expansions
and revisions can be expected.
- Galactars are holispheres bound to a masscentre and inside a gravitysheath.
- Galactar holispheres consist of all types of object from galaxies downward.
- Galactars contain up to around a thousand galaxies.
- Galactar masses are up to around 1015 solarmasses.
- Galactar mass is 90% subphotonic darkmatter.
- Galactar diameters are up to around 5mpc.
GALACTARS IN CORE PHYSICS
Nothing in the galactar factbase clashes with Core
Physics expectations. These extrapolations from the Core Physics
Taxonomic Table may provide insight.
- Each galaxy in a galactar has its own gravitysheath.
- Each galaxy in a galactar is in dominance adjacency inside the galactar gravitysheath.
- Each galaxy in a galactar is in type adjacency to adjacent galaxies.
- Each galactar is inside its own gravitysheath.
- Galactars inside the gravitysheath of another galactar are in dominance adjacency.
- Galactars in dominance adjacency and below escape velocity are dissipated and absorbed over time.
- Galactar holispheres consist of all types of object from stars downward.
- Galactars observed by photon emission are understable at the time of emission.
- Galactars unobservable by photon emission may, or may not, be understable.
- Understable galactars undergo accretion expansion.
- Understable galactars undergo stabilisation contraction.
- Understable galactars stabilise per the energy/mass differential.
- The mass of a galactar is such that it has a central event horizon.
CAVEAT
The endpoint in the lifecycle of a galactar is either being
accreted or becoming stable - stable being without any ejections,
emissions, or expulsions. It may be that no galactar in the visible
universe has yet stabilised.
CAVEAT
Large aggregations of galaxies are observed that exceed what is
currently considered to be a galactar. Whether these are larger
galactars or clusters of galactars is unclear. Just as there seems to
be an upper limit to the mass and/or size of understable
hypergiantstars, there may be a limit to the mass and/or size of
understable galactars. However, there is currently nothing (in Core
Physics) that prevents galactars coming together as galactar
clusters. That is: as a cluster of type adjacent galactars bound by
their mutual gravitypull inside is own gravitysheath. The mass of
a galactar cluster would be such that there would be an event
horizon at its centre.
CAVEAT
Everything known in the Universe stabilises if conditions
allow. For a galactar, stabilisation requires the ejection of a
significant proportion of its energy and mass after peakmass. This
creates a vicious circle.
- Ejections from understable galactars are into the gravitysheaths of adjacent galactars.
- Thus understable galactars are absorbing the ejections of adjacent galactars.
- Thus stabilising galaxies are simultaneously absorbing and ejecting.
- Thus galactars cannot stabilise.
The
vicious circle is only broken if the Universe is seen as a spheroidal
galactar cluster beyond which there is a region of space. The
galactars on the outside of the Universe would eject their excess of
energy and mass into that space and thus be the exhaust allowing
all the galactars to stabilise eventually.
Notably, the
ejected mass would become a holisphere for the spheroid which would
grow in mass as the the galactars stabilised. The gravitypull of the
holisphere would have exactly the effect on the spheroid that is
currently attributed to darkenergy.
So is the Universe a spheroid of galactars. Possibly. But probably not. See the next caveat.
CAVEAT
An important lesson to be taken from the current Core
Physics taxonomy is that, just as the notion that the Earth is the
centre of the Universe was abandoned, the notion that humans occupy the
centre point in the taxonomic table should be abandoned also.
The
mechanics of gravitypull and repellence are not explained by
positing a teel universe. It is therefore reasonable to
suppose the explanations for gravitypull and repellence will be
found in pre-teel cumulations. This may mean there is just one taxon
below that of teels but that cannot be assumed.
Similarly, the
current description of the larger universe is effectively bounded by
what can be seen. However, the Core Physics taxonomy is constructed out
of a very small set of rules. There is no good reason to suppose that
the universe that cannot be seen is not subject to exactly the same
rules.
The previous caveat hypothesised the universe as a
spheroid of galactars. That is a possibility although not the only
possibility. What is also a possibility, actually more a
likelihood, is that the Universe is part of a uberuniverse operating
under the same fundamental rules already empirically verified.
As
to what that the structure of the uberuniverse might be, as of
now, an open question. Answers may be forthcoming if it
can be determined what the Universe will be when it has
stabilised. Will it be an independent object like a molecule in an
atmosphere. Or will it be a subsidiary unit in a larger object like a
quark in a nucleon. Time will tell us. Or it will not. |
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.
* * * * *
Hypergianstars
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 precollapse already have a darksphere
surrounding their gravitycentre. Certainly, the postcollapse
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-mementum teelocean. Objects drawn into the teeloceon 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, undestable 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 galactiv |
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Copyright 2022 - Sian Luise Winchester
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