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Taxon 4.3
FERRICNUCLIDES
| Stableable isotopes of elements 26 to 82 which absorb more energy during manufacture than they eject. |
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Work in progress
Taxon 4.3 Stableable isotopes of elements 26 to 82 which absorb more energy during manufacture than they eject. Taxonome 4.3.1
Understable isotopes of elements 26 to (currently) 118
which directly or indirectly to stableable isotope of 82 or less as conditions dictate. |
Notes on the structure of nuclides:
- nuclides are two or more strongforced nucleons.
- strongforcing is the mutual gravitypull of the nucleon nucleuses countered by the mutual masspushes of the nucleon teelstreams.
- the masspushing nucleon teelstreams are (probably) teeloceans.
- the teelocean streams are driven (ultimately) by the spins of the nucleon quarks.
- the configuration of the nucleons within a nuclide is not fixed.
- the configuration is that of least stress.
- the
configuration can alter because the nucleons "float" on each
others teeloceans and are thus able to slide from one position to
another.
- "float"
does not mean that each teelocean is distinct. Within each nucleons
gravitysheath, the teelocean is its own but the nucleons are engorged
and thus understable. There is a constant interchange of teels from one
gravitysheath to another. The teeloceans are perhaps best seen as the
teelocean of the nuclide within and through which a complex of
teelstream systems is in constant motion.
- the least stressful configuration is dictated by the teelocean teelstreams.
- the teelstreams of protons are axial and those of neutrons are centrifugal.
- because
the nucleons in a nuclide are engorged, each is continually absorbing
and ejecting teels, the protons ejecting at their northpoles and the
neutrons ejecting at their equators.
- the
engorgement of the nucleons overrides their possession of their own
teeloceans which flow in between the nucleon nucleuses to be the
nuclide teelocean stream system.
- for any given number of nucleons in a nuclide there is a pattern to the nuclide teelocean system that is least stressful.
- the least stressful teelocean system requires the "floating" nucleons to adopt their own least stressful configuration.
- the nucleon configuration is also nucleon type specific.
- protons will transmute to neutrons and neutrons will transmute to protons as necessary to minimise the teelocean stress.
- NB:
further consideration to be given to whether, in larger nuclides, the
least stressful configuration requires forming the nucleons into
heliums.
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Ferricnuclides
() Ferricnuclides are a multicore nucleus inside a teelosphere inside a gravitysheath inside a gravitysheath interface. () Ferricnuclide nucleuses primarily contain numbers of helium-4. () Some ferricnuclide nucleuses contain nucleons. () Ferricnuclide nucleus content is strongforced. () Ferricnuclides are manufactured in star nucleuses () Ferricnuclide are divided into elements. () Ferricnuclide elements are (1) iron to oganesson. () Ferricnuclide elements are (2) elementnumbers 26 to 118. () Ferricnuclide elements are divided into isotopes. () Ferricnuclide isotopes are typified by isotopenumber. () Ferricnuclide elements are whiteferrics and blackferrics. () Whiteferric elements have at least one stable isotope. () Whiteferrics are (1) iron to lead. () Whiteferrics are (2) elementnumbers 26 to 82. () Blackferric elements have no stable isotopes. () Blackferrics are (1) bismuth to oganesson. () Blackferrics are (2) elementnumbers 83 to 118.
Mechanics
() Ferricnuclides stratify in stars by elementnumber. () Elementnumber stratification is lowest outward as conditions permit.Manufacture by fusion Absorption / ejection differential
- Fusions result in absorption of additional gravitymass.
- Successive fusions result in successive increases in gravitymass.
- Each gravitymass increase is between neutron and helium gravitymass.
- Gravitymass increase results in attunement loss.
- Attunement is regained by ejecting gravitymass.
- Lithicnuclide attunements require ejecting more gravitymass than is absorbed.
- Successive fusions require successively less gravitymass ejection to regain attunement.
- Fusions of lithium isotopes require the greatest gravitymass ejections.
- Fusions of manganese isotopes require the least ejections.
- Ferricnuclide attunements require less ejection of gravitymass than is absorbed.
() Ferricnuclides are manufactured in star nucleuses. () Ferricnuclides are manufactured by fusion of stripped nucleons / heliums with cationised nuclides. () Ferricnuclide fusions absorb more gravitymassvelocity than is ejected. () Ferricnuclides are elements iron to oganesson. () Ferricnuclides are elementnumbers 26 to 118. () Elementnumbers 26 to 82 are whiteferric nuclides. () Elementnumbers 83 to 118 are blackferric nuclides.
() Stellar ferricnuclide isotopes are engorged. () Stellar ferricnuclide isotopes are overstable, stableable, or understable. () Stellar ferricnuclide isotopes made overstable during fusions become understable by absorbing substrate. () Stellar whiteferric isotopes do not decay. () Stellar blackferric isotopes are not stableable. () Stellar blackferric isotopes - some types spontaneous fissiondecay in criticalmass. () Stellar blackferric isotopes - some types induced fissiondecay if conditions dictate.
() Non stellar whiteferric isotopes are stable, stableable or understable. () Non stellar blackferric isotopes are all understable. () Non stellar understable ferricnuclide isotopes decay to stable or stableable isotopes. () Nonstellar understable whiteferric isotope decays are alphadecay, betadecay, and nucleondecay. () Nonstellar understable blackferric isotope decays are alphadecay, betadecay, nucleondecay, and fissiondecay.
(2a) Ferricnuclide fusion results in ferricnuclide isotopes absorbing more gravitymassvelocity than is ejected or emitted. (2b) The difference between absorption and ejection /emission results in ferriccollapse. (2c) Ferriccollapse contracts the fusing isotope stratums. (2d) Ferriccollapse overengorges ferricnuclide isotope nucleons. (2e) Overengorged protons transmute to neutrons. (2f) Neutrons are stripped by the increasing intrinsic gravitypull. (2g) Neutron stripment ejects teels from the ferricnuclide stratums. (2h) Ejected teels eject the lithicnuclide stratums from the star. (2i) Ferriccollapse has contracted the ferricnuclide stratums to a neutronstar.
(3a) Ferriccollapse is the primary semistabilisation mechanism in whitestars. (3b) Ferriccollapse is a secondary semistabilisation mechanism in blackstars.
(2a) Ferricnuclides are a multicore nucleus inside a teelosphere inside a gravitysheath. (2b) Ferricnuclides nucleuses consist of numbers of strongforced nucleons. (2c) Ferricnuclides are manufactured in stars.
(3a) Ferricnuclides are the elements iron to oganesson. (3b) Ferricnuclides are elementnumbers 26 to 118. (3c) Ferricnuclide elements have isotopes. (3d) Ferricnuclide elements iron (26) to lead (82) have stable and understable isotopes. (3e) Ferricnuclide elements (83) bismuth to oganesson (118) have only understable isotopes.
(4a) Understable isotopes decay to another isotope. (4b) Understable isotopes are whiteferric or blackferric. (4c) Whiteferric isotope decays are alphadecay, betadecay, nucleondecay. (4d) Blackferric isotope decays are also induced fissiondecay, spontaneous fissiondecay.
(5a) Ferricnuclide manufacture is by fusion with stripped neutrons and stripped heliums. (5b) Each additional fusion absorbs more gravitymassvelocity than is ejected or emitted. (5c) Each additional fusion increases elementnumber and/or neutronnumber. (5d) Rule of thumb: increases in elementnumber are overall exceeded by increases in neutronnumber. (5e) Excess neutrons are stripped to form a neutroncore inside a Helium-4 shell.
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©2024 - Ed Winchester / Sian Winchester
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SUPERCEDED MATTER
BLACKFERRIC A ferricnuclide element that has no stable isotopes.
WHITEFERRIC A ferricnuclide element that has at least one stable isotope.
() Ferricnuclides are manufactured in star nucleuses. () Ferricnuclides are manufactured by fusion of stripped nucleons / heliums with cationised nuclides. () Ferricnuclide fusions absorb more gravitymassvelocity than is ejected. () Ferricnuclides are elements iron to oganesson. () Ferricnuclides are elementnumbers 26 to 118. () Elementnumbers 26 to 82 are whiteferric nuclides. () Elementnumbers 83 to 118 are blackferric nuclides.
() Stellar ferricnuclide isotopes are engorged. () Stellar ferricnuclide isotopes are overstable, stableable, or understable. () Stellar ferricnuclide isotopes made overstable during fusions become understable by absorbing substrate. () Stellar whiteferric isotopes do not decay. () Stellar blackferric isotopes are not stableable. () Stellar blackferric isotopes - some types spontaneous fissiondecay in criticalmass. () Stellar blackferric isotopes - some types induced fissiondecay if conditions dictate.
() Non stellar whiteferric isotopes are stable, stableable or understable. () Non stellar blackferric isotopes are all understable. () Non stellar understable ferricnuclide isotopes decay to stable or stableable isotopes. () Nonstellar understable whiteferric isotope decays are alphadecay, betadecay, and nucleondecay. () Nonstellar understable blackferric isotope decays are alphadecay, betadecay, nucleondecay, and fissiondecay.
(2a) Ferricnuclides are a multicore nucleus inside a teelosphere inside a gravitysheath. (2b) Ferricnuclides nucleuses consist of numbers of strongforced nucleons. (2c) Ferricnuclides are manufactured in stars.
(3a) Ferricnuclides are the elements iron to oganesson. (3b) Ferricnuclides are elementnumbers 26 to 118. (3c) Ferricnuclide elements have isotopes. (3d) Ferricnuclide elements iron (26) to lead (82) have stable and understable isotopes. (3e) Ferricnuclide elements (83) bismuth to oganesson (118) have only understable isotopes.
(4a) Understable isotopes decay to another isotope. (4b) Understable isotopes are whiteferric or blackferric. (4c) Whiteferric isotope decays are alphadecay, betadecay, nucleondecay. (4d) Blackferric isotope decays are also induced fissiondecay, spontaneous fissiondecay.
(5a) Ferricnuclide manufacture is by fusion with stripped neutrons and stripped heliums. (5b) Each additional fusion absorbs more gravitymassvelocity than is ejected or emitted. (5c) Each additional fusion increases elementnumber and/or neutronnumber. (5d) Rule of thumb: increases in elementnumber are overall exceeded by increases in neutronnumber. (5e) Excess neutrons are stripped to form a neutroncore inside a Helium-4 shell. |
| FERRICNUCLIDES - DESCRIPTION |
Ferricnuclides = A ferricnuclide is a nuclidic nucleus inside a teelosphere =Ferricnuclides are ranges of ferricnuclide elements =- Elements are typified by the number of protons in the nucleus =
- Elements are either uranic or transuranic =
- Transuranic elements do not occur naturally on Earth =
- From Neptunium (93 protons) to Oganesson (118 protons) =
- These elements have been synthesised on Earth =
- Elements with more than 118 protons may or may not be synthesised in future.
Ferricnuclide elements are ranges of element isotopes =- Isotopes are typified by the number of neutrons in the nucleus =
- Rule
of thumb: as the mass of ferricnuclide isotopes increase, the number of
neutrons increasingly exceeds the number of protons.
- Neutroncores form at the centre of the nucleus from the excess neutrons.
Ferricnuclide element isotopes are stable or understable =
- Stable isotopes have the same energyvelocity and massvelocity =
- Thus =
- Stable isotopes do not decay =
- Elements between Iron (26 protons) and Lead (82 protons) have at least one stable isotope.
- Elements between Bismuth (83 protons) and Oganesson (118 protons) have only understable isotopes.
- Understable isotopes have more energyvelocity than massvelocity =
- Thus =
- Understable isotopes decay.
Understable element isotopes undergo a range of decay types =- Decay is the change of an understable isotope to another isotope and/or element by the ejection of energymass =
- The decay type undergone depends on the isotope type =
- Thus: changing isotope and/or element type.
- Nucleondecay =
- Ejecting one or more nucleons.
- Thus: changing isotope and element type.
- Thus: becoming two or more lesser element types.
- There are two types of fissiondecay =
- Spontaneous fissiondecay =
- When the nucleus splits unpredictably with no apparent cause.
- Induced fissiondecay =
- When the nucleus splits after neutron absorption from an adjacent spontaneous fissiondecay.
Ferricnuclides are made of numbers of heliums =- Helium nuclei are two neutrons and two protons =
- Helium nuclei are strongly bound and maintain their form =
- Ferricnuclides have more neutrons than protons =
Ferricnuclide neutroncores are at the centre of the nuclidic nucleus =
Ferricnuclides are manufactured in stars.
- Fusion of increasingly massive ferricnuclide isotopes =
- May or may not be by the fusion of two or more nuclides.
- May or may not be by the fusion of nuclides with stripped neutrons and/or stripped heliums.
- Assumption =
- Fusion
of increasingly massive ferricnuclide isotopes is by the fusion of
nuclides with stripped neutrons and/or stripped heliums.
- Ferricnuclide fusions =
- The more massive the fused ferricnuclide, the greater the disparity between the before and after energymass.
- Ferricnuclide elements up to Lead (82 protons) =
- Ferricnuclide elements beyond Lead (83 protons and up) =
- Have only understable isotopes.
- Ferricnuclide elements up to Protactinium (91 protons) =
- Ferricnuclide elements beyond Protactinium (92 protons) =
- Increasing stellar peakmass increases stellar intrinsic gravitypull =
| EARLIER MATERIAL FOR REVISION AND INCLUSION AS APPROPRIATE |
FERRICCOLLAPSE
Ferric core contraction does not happen in dwarfstars. It is the major cause of contraction in giantstars. It is a precursor to collapse in supergiantstars and hypergiantstars.
As long as stars are understable they are contracting because they are differentially ejecting energy and mass (see: energy/mass differential). Rule of thumb: before peakmass stabilisation contraction is dominated by accretion expansion. After peakmass, stabilisation contraction dominates accretion expansion.
* * * * *
Isotopes are bound into stars by intrinsic gravitypull. Adjacent isotopes are prevented from strongforcing by the repellence of their
engorged teelospheres. This repellence is reinforced by the emission pressure
of engorgement photons and fusion photons.At a given peakmass stars begin to fuse ferric isotopes. In ferric isotopes the excess of mutual repellence over mutual gravitypull is already significantly decreased, as is the emission pressure. Now the decreases are reinforced by absorbing stripped neutrons into a neutron core. This is accretion and not fusion. Thus mass is increased without any photon emission. No photon emission equates to no effect on emission pressure.Each ferric isotope mass increase:The rate of ferric core contraction is tied to star peakmass. The
higher the peakmass, the faster the contraction. In high peakmass
stars the contraction rate is impressively rapid.
The contraction of a ferric core is a converging of its ferric isotope nuclei. Simultaneously, the nuclei grow in volume as they increase in mass. Consequently, progressively less room is left between the nuclei for their teelospheres. This results in teels being expelled from the ferric core at an increasing rate. The loss of teelospheres is a loss of repellence.
The
teels are expelled from the ferric core into the surrounding subferric stratums. The teels further engorge the subferric isotopes and accelerate them away from the ferric core. Low
peakmass stars have a low contraction rate but it is still enough to expel
some subferric isotopes out of their stars. High peakmass
stars with their high contraction rates can expel everything outside
the ferric
core.
FERRICCORE EXPULSION
As long as stars are understable they are contracting because they are stabilising by ejecting energy and mass per the energy/mass differential. Before peakmass, stabilisation contraction is dominated by accretion expansion. After peakmass, stabilisation contraction dominates accretion expansion.
In the ferric cores of giantstars, supergiantstars, and hypergiantstars stabilisation contraction is reinforced by the absorbing of stripped neutrons into the neutron cores of ferric isotopes. This is accretion, not fusion, so the mass of the ferric isotopes increases without photon emissions and thus no alteration in emission pressure.Converging the ferric isotope nuclei leaves less room for their teelospheres.The teels are expelled into the surrounding stratums of subferric isotopes. The already engorged subferric isotopes are further engorged by the teels and accelerated away from the ferric core. Some or all of the subferric isotopes are expelled from the star. The highest peakmass stars expel everything outside the ferric core.
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