Search This Blog

Monday, October 30, 2023

Expanding Earth

From Wikipedia, the free encyclopedia
Historical Hilgenberg globes
Potential reconstruction of continents bordering the Atlantic (left column) and Pacific (right column) oceans as they might have appeared at different points, going back in history, using the expanding Earth hypothesis, based on reconstructions by expanding Earth proponent Neal Adams

The expanding Earth or growing Earth hypothesis argues that the position and relative movement of continents is due at least partially to the volume of Earth increasing. Conversely, geophysical global cooling was the hypothesis that various features could be explained by Earth contracting.

Although it was suggested historically, since the recognition of plate tectonics during the mid 20th century, scientific consensus has rejected the idea of any significant expansion or contraction of Earth.

Different forms of the hypothesis

Expansion with constant mass

In 1834, during the second voyage of HMS Beagle, Charles Darwin investigated stepped plains featuring raised beaches in Patagonia which indicated to him that a huge area of South America had been "uplifted to its present height by a succession of elevations which acted over the whole of this space with nearly an equal force". While his mentor Charles Lyell had suggested forces acting near the crust on smaller areas, Darwin hypothesized that uplift at this continental scale required "the gradual expansion of some central mass" [of the Earth] "acting by intervals on the outer crust" with the "elevations being concentric with form of globe (or certainly nearly so)". In 1835 he extended this concept to include the Andes Mountains as part of a curved enlargement of the Earth's crust due to "the action of one connected force". Not long afterwards, he abandoned this idea and proposed that as the mountains rose, the ocean floor subsided, explaining the formation of coral reefs.

In 1889 and 1909 Roberto Mantovani published a hypothesis of Earth expansion and continental drift. He assumed that a closed continent covered the entire surface of a smaller Earth. Thermal expansion caused volcanic activity, which broke the land mass into smaller continents. These continents drifted away from each other because of further expansion at the rip-zones, where oceans currently lie. Although Alfred Wegener noticed some similarities to his own hypothesis of continental drift, he did not mention Earth expansion as the cause of drift in Mantovani's hypothesis.

A compromise between Earth-expansion and Earth-contraction is the "theory of thermal cycles" by Irish physicist John Joly. He assumed that heat flow from radioactive decay inside Earth surpasses the cooling of Earth's exterior. Together with British geologist Arthur Holmes, Joly proposed a hypothesis in which Earth loses its heat by cyclic periods of expansion. By their hypothesis, expansion caused cracks and joints in Earth's interior that could fill with magma. This was succeeded by a cooling phase, where the magma would freeze and become solid rock again, causing Earth to shrink.

Mass addition

In 1888 Ivan Osipovich Yarkovsky suggested that some sort of aether is absorbed within Earth and transformed into new chemical elements, forcing the celestial bodies to expand. This was associated with his mechanical explanation of gravitation. Also the theses of Ott Christoph Hilgenberg (1933, 1974) and Nikola Tesla (1935) were based on absorption and transformation of aether-energy into normal matter.

Samuel Warren Carey

After initially endorsing the idea of continental drift, Australian geologist Samuel Warren Carey advocated expansion from the 1950s (before the idea of plate tectonics was generally accepted) to his death, alleging that subduction and other events could not balance the sea-floor spreading at oceanic ridges, and describing yet unresolved paradoxes that continue to plague plate tectonics. Starting in 1956, he proposed some sort of mass increase in the planets and said that a final solution to the problem is only possible by cosmological processes associated with the expansion of the universe.

Bruce Heezen initially interpreted his work on the mid-Atlantic ridge as confirming S. Warren Carey's Expanding Earth Theory, but later ended his endorsement, finally convinced by the data and analysis of his assistant, Marie Tharp. The remaining proponents after the 1970s, like the Australian geologist James Maxlow, are mainly inspired by Carey's ideas.

To date no scientific mechanism of action has been proposed for this addition of new mass. Although the earth is constantly acquiring mass through accumulation of rocks and dust from space such accretion, however, is only a minuscule fraction of the mass increase required by the growing earth hypothesis.

Decrease of the gravitational constant

Paul Dirac suggested in 1938 that the universal gravitational constant had decreased during the billions of years of its existence. This caused German physicist Pascual Jordan to propose in 1964, a modification of the theory of general relativity, that all planets slowly expand. This explanation is considered a viable hypothesis within the context of physics.

Measurements of a possible variation of the gravitational constant showed an upper limit for a relative change of 5×10−12 per year, excluding Jordan's idea.

Formation from a gas giant

According to the hypothesis of J. Marvin Herndon (2005, 2013) the Earth originated in its protoplanetary stage from a Jupiter-like gas giant. During the development phases of the young Sun, which resembled those of a T Tauri star, the dense atmosphere of the gas giant was stripped off by infrared eruptions from the sun. The remnant was a rocky planet. Due to the loss of pressure from its atmosphere it would have begun a progressive decompression. Herndon regards the energy released due to the lack of compression as a primary energy source for geotectonic activity, to which some energy from radioactive decomposition processes was added. He terms the resulting changes in the course of Earth's history by the name of his theory Whole-Earth Decompression Dynamics. He considered seafloor spreading at divergent plate boundaries as an effect of it. In his opinion mantle convection as used as a concept in the theory of plate tectonics is physically impossible. His theory includes the effect of solar wind (geomagnetic storms) as cause for the reversals of the Earth magnetic field. The question of mass increase is not addressed.

Main arguments against Earth expansion

The hypothesis had never developed a plausible and verifiable mechanism of action. During the 1960s, the theory of plate tectonics— based initially on the assumption that Earth's size remains constant, and relating the subduction zones to burying of lithosphere at a scale comparable to seafloor spreading—became the accepted explanation in the Earth Sciences.

The scientific community finds that significant evidence contradicts the Expanding Earth theory, and that the evidence used for it is explained better by plate tectonics:

  • Measurements with modern high-precision geodetic techniques and modeling of the measurements by the horizontal motions of independent rigid plates at the surface of a globe of free radius, were proposed as evidence that Earth is not currently increasing in size to within a measurement accuracy of 0.2 mm per year. The main author of the study stated "Our study provides an independent confirmation that the solid Earth is not getting larger at present, within current measurement uncertainties".
  • The motions of tectonic plates and subduction zones measured by a large range of geological, geodetic and geophysical techniques helps verify plate tectonics.
  • Imaging of lithosphere fragments within the mantle is evidence for lithosphere consumption by subduction.
  • Paleomagnetic data has been used to calculate that the radius of Earth 400 million years ago was 102 ± 2.8 percent of the present radius.
  • Examinations of data from the Paleozoic and Earth's moment of inertia suggest that there has not been any significant change of Earth's radius during the last 620 million years.

List of particles

From Wikipedia, the free encyclopedia
https://en.wikipedia.org/wiki/List_of_particles

This is a list of known and hypothesized particles.

Standard Model elementary particles

Elementary particles are particles with no measurable internal structure; that is, it is unknown whether they are composed of other particles. They are the fundamental objects of quantum field theory. Many families and sub-families of elementary particles exist. Elementary particles are classified according to their spin. Fermions have half-integer spin while bosons have integer spin. All the particles of the Standard Model have been experimentally observed, including the Higgs boson in 2012. Many other hypothetical elementary particles, such as the graviton, have been proposed, but not observed experimentally.

Fermions

Fermions are one of the two fundamental classes of particles, the other being bosons. Fermion particles are described by Fermi–Dirac statistics and have quantum numbers described by the Pauli exclusion principle. They include the quarks and leptons, as well as any composite particles consisting of an odd number of these, such as all baryons and many atoms and nuclei.

Fermions have half-integer spin; for all known elementary fermions this is 12. All known fermions except neutrinos, are also Dirac fermions; that is, each known fermion has its own distinct antiparticle. It is not known whether the neutrino is a Dirac fermion or a Majorana fermion. Fermions are the basic building blocks of all matter. They are classified according to whether they interact via the strong interaction or not. In the Standard Model, there are 12 types of elementary fermions: six quarks and six leptons.

Quarks

Quarks are the fundamental constituents of hadrons and interact via the strong force. Quarks are the only known carriers of fractional charge, but because they combine in groups of three quarks (baryons) or in pairs of one quark and one antiquark (mesons), only integer charge is observed in nature. Their respective antiparticles are the antiquarks, which are identical except that they carry the opposite electric charge (for example the up quark carries charge +23, while the up antiquark carries charge −23), color charge, and baryon number. There are six flavors of quarks; the three positively charged quarks are called "up-type quarks" while the three negatively charged quarks are called "down-type quarks".

Quarks
Generation Name Symbol Antiparticle Spin Charge
(e)
Mass (MeV/c2
1 up u
u
12 +23 2.2+0.6
−0.4
down d
d
12 13 4.6+0.5
−0.4
2 charm c
c
12 +23 1280±30
strange s
s
12 13 96+8
−4
3 top t
t
12 +23 173100±600
bottom b
b
12 13 4180+40
−30

Leptons

Leptons do not interact via the strong interaction. Their respective antiparticles are the antileptons, which are identical, except that they carry the opposite electric charge and lepton number. The antiparticle of an electron is an antielectron, which is almost always called a "positron" for historical reasons. There are six leptons in total; the three charged leptons are called "electron-like leptons", while the neutral leptons are called "neutrinos". Neutrinos are known to oscillate, so that neutrinos of definite flavor do not have definite mass, rather they exist in a superposition of mass eigenstates. The hypothetical heavy right-handed neutrino, called a "sterile neutrino", has been omitted.

Leptons
Generation Name Symbol Antiparticle Spin Charge
(e)
Mass (MeV/c2
1 electron
e

e+
1/2 −1 0.511
electron neutrino
ν
e

ν
e
1/2 0 < 0.0000022
2 muon
μ

μ+
1/2 −1 105.7
muon neutrino
ν
μ

ν
μ
1/2 0 < 0.170
3 tau
τ

τ+
1/2 −1 1776.86±0.12
tau neutrino
ν
τ

ν
τ
1/2 0 < 15.5

Bosons

Bosons are one of the two fundamental particles having integral spinclasses of particles, the other being fermions. Bosons are characterized by Bose–Einstein statistics and all have integer spins. Bosons may be either elementary, like photons and gluons, or composite, like mesons.

According to the Standard Model, the elementary bosons are:

Name Symbol Antiparticle Spin Charge (e) Mass (GeV/c2 Interaction mediated Observed
photon γ self 1 0 0 electromagnetism Yes
W boson
W

W+
1 ±1 80.385±0.015 weak interaction Yes
Z boson
Z
self 1 0 91.1875±0.0021 weak interaction Yes
gluon
g
self 1 0 0 strong interaction Yes
Higgs boson
H0
self 0 0 125.09±0.24 mass Yes

The Higgs boson is postulated by the electroweak theory primarily to explain the origin of particle masses. In a process known as the "Higgs mechanism", the Higgs boson and the other gauge bosons in the Standard Model acquire mass via spontaneous symmetry breaking of the SU(2) gauge symmetry. The Minimal Supersymmetric Standard Model (MSSM) predicts several Higgs bosons. On 4 July 2012, the discovery of a new particle with a mass between 125 and 127 GeV/c2 was announced; physicists suspected that it was the Higgs boson. Since then, the particle has been shown to behave, interact, and decay in many of the ways predicted for Higgs particles by the Standard Model, as well as having even parity and zero spin, two fundamental attributes of a Higgs boson. This also means it is the first elementary scalar particle discovered in nature.

Elementary bosons responsible for the four fundamental forces of nature are called force particles (gauge bosons). Strong interaction is mediated by the gluon, weak interaction is mediated by the W and Z bosons.

Hypothetical particles

Graviton

Name Symbol Antiparticle Spin Charge (e) Mass (GeV/c2 Interaction mediated Observed
graviton G self 2 0 0 gravitation No

The graviton is a hypothetical particle that has been included in some extensions to the standard model to mediate the gravitational force. It is in a peculiar category between known and hypothetical particles: As an unobserved particle that is not predicted by, nor required for the Standard Model, it belongs in the table of hypothetical particles, below. But gravitational force itself is a certainty, and expressing that known force in the framework of a quantum field theory requires a boson to mediate it.

If it exists, the graviton is expected to be massless because the gravitational force has a very long range, and appears to propagate at the speed of light. The graviton must be a spin-2 boson because the source of gravitation is the stress–energy tensor, a second-order tensor (compared with electromagnetism's spin-1 photon, the source of which is the four-current, a first-order tensor). Additionally, it can be shown that any massless spin-2 field would give rise to a force indistinguishable from gravitation, because a massless spin-2 field would couple to the stress–energy tensor in the same way that gravitational interactions do. This result suggests that, if a massless spin-2 particle is discovered, it must be the graviton.

Particles predicted by supersymmetric theories

Supersymmetric theories predict the existence of more particles, none of which have been confirmed experimentally.

Superpartners (Sparticles)
Superpartner Spin Notes superpartner of:
chargino
 1 /2
The charginos are superpositions of the superpartners of charged Standard Model bosons: charged Higgs boson and W boson.
The MSSM predicts two pairs of charginos.
charged bosons
gluino
 1 /2
Eight gluons and eight gluinos. gluon
gravitino
 3 /2
Predicted by supergravity (SUGRA). The graviton is hypothetical, too – see previous table. graviton
Higgsino
 1/ 2
For supersymmetry there is a need for several Higgs bosons, neutral and charged, according with their superpartners. Higgs boson
neutralino
 1 /2
The neutralinos are superpositions of the superpartners of neutral Standard Model bosons: neutral Higgs boson, Z boson and photon.
The lightest neutralino is a leading candidate for dark matter.
The MSSM predicts four neutralinos.
neutral bosons
photino
 1 /2
Mixing with zino and neutral Higgsinos for neutralinos. photon
sleptons
0
The superpartners of the leptons (electron, muon, tau) and the neutrinos. leptons
sneutrino
0
Introduced by many extensions of the Standard Supermodel, and may be needed to explain the LSND results.
A special role has the sterile sneutrino, the supersymmetric counterpart of the hypothetical right-handed neutrino, called the "sterile neutrino".
neutrino
squarks
0
The stop squark (superpartner of the top quark) is thought to have a low mass and is often the subject of experimental searches. quarks
wino, zino
 1 /2
The charged wino mixing with the charged Higgsino for charginos, for the zino see line above. W± and Z0 bosons

Just as the photon, Z boson and W± bosons are superpositions of the B0, W0, W1, and W2 fields, the photino, zino, and wino± are superpositions of the bino0, wino0, wino1, and wino2. No matter if one uses the original gauginos or this superpositions as a basis, the only predicted physical particles are neutralinos and charginos as a superposition of them together with the Higgsinos.

Other hypothetical bosons and fermions

Other theories predict the existence of additional elementary bosons and fermions, with some theories also postulating additional superpartners for these particles:

Other hypothetical bosons and fermions
Name Spin Notes
axion
0
A pseudoscalar particle introduced in Peccei–Quinn theory to solve the strong-CP problem.
axino
 1 /2
Superpartner of the axion. Forms a supermultiplet, together with the saxion and axion, in supersymmetric extensions of Peccei–Quinn theory.
branon
?
Predicted in brane world models.
digamma
?
Proposed resonance of mass near 750 GeV that decays into two photons.
dilaton
0
Predicted in some string theories.
dilatino
 1 /2
Superpartner of the dilaton.
dual graviton
2
Has been hypothesized as dual of graviton under electric–magnetic duality in supergravity.
graviphoton
1
Also known as "gravivector".
graviscalar
0
Also known as "radion".
inflaton
0
Unidentified scalar force-carrier that is presumed to have physically caused cosmological “inflation” – the rapid expansion from 10−35 to 10−34 seconds after the Big Bang.
magnetic photon
?
Predicted in 1966.
majoron
0
Predicted to understand neutrino masses by the seesaw mechanism.
majorana fermion  1 /2;  3 /2 ? ... gluino, neutralino, or other – is its own antiparticle.
saxion
0

X17 particle
?
possible cause of anomalous measurement results near 17 MeV, and possible candidate for dark matter.
X and Y bosons
1
These leptoquarks are predicted by GUT theories to be heavier equivalents of the W and Z.
W′ and Z′ bosons
1

Other hypothetical elementary particles

Composite particles

Composite particles are bound states of elementary particles.

Hadrons

Hadrons are defined as strongly interacting composite particles. Hadrons are either:

Quark models, first proposed in 1964 independently by Murray Gell-Mann and George Zweig (who called quarks "aces"), describe the known hadrons as composed of valence quarks and/or antiquarks, tightly bound by the color force, which is mediated by gluons. (The interaction between quarks and gluons is described by the theory of quantum chromodynamics.) A "sea" of virtual quark-antiquark pairs is also present in each hadron.

Baryons

A combination of three u, d or s-quarks with a total spin of 32 form the so-called "baryon decuplet".
Proton quark structure: 2 up quarks and 1 down quark.

Ordinary baryons (composite fermions) contain three valence quarks or three valence antiquarks each.

  • Nucleons are the fermionic constituents of normal atomic nuclei:
    • Protons, composed of two up and one down quark (uud)
    • Neutrons, composed of two down and one up quark (ddu)
  • Hyperons, such as the Λ, Σ, Ξ, and Ω particles, which contain one or more strange quarks, are short-lived and heavier than nucleons. Although not normally present in atomic nuclei, they can appear in short-lived hypernuclei.
  • A number of charmed and bottom baryons have also been observed.
  • Pentaquarks consist of four valence quarks and one valence antiquark.
  • Other exotic baryons may also exist.

Mesons

Mesons of spin 0 form a nonet.

Ordinary mesons are made up of a valence quark and a valence antiquark. Because mesons have integer spin (0 or 1) and are not themselves elementary particles, they are classified as “composite“ bosons, although being made of elementary fermions. Examples of mesons include the pion, kaon, and the J/ψ. In quantum hadrodynamics, mesons mediate the residual strong force between nucleons.

At one time or another, positive signatures have been reported for all of the following exotic mesons but their existences have yet to be confirmed.

  • A tetraquark consists of two valence quarks and two valence antiquarks;
  • A glueball is a bound state of gluons with no valence quarks;
  • Hybrid mesons consist of one or more valence quark–antiquark pairs and one or more real gluons.

Atomic nuclei

A semi-accurate depiction of the helium atom. In the nucleus, the protons are in red and neutrons are in purple. In reality, the nucleus is also spherically symmetrical.

Atomic nuclei typically consist of protons and neutrons, although exotic nuclei may consist of other baryons, such as hypertriton which contains a hyperon. These baryons (protons, neutrons, hyperons, etc.) which comprise the nucleus are called nucleons. Each type of nucleus is called a "nuclide", and each nuclide is defined by the specific number of each type of nucleon.

  • "Isotopes" are nuclides which have the same number of protons but differing numbers of neutrons.
  • Conversely, "isotones" are nuclides which have the same number of neutrons but differing numbers of protons.
  • "Isobars" are nuclides which have the same total number of nucleons but which differ in the number of each type of nucleon. Nuclear reactions can change one nuclide into another.

Atoms

Atoms are the smallest neutral particles into which matter can be divided by chemical reactions. An atom consists of a small, heavy nucleus surrounded by a relatively large, light cloud of electrons. An atomic nucleus typically consists of 1 or more protons and 0 or more neutrons. Protons and neutrons are, in turn, made of quarks. Each type of atom corresponds to a specific chemical element. To date, 118 elements have been discovered or created.

Exotic atoms may be composed of particles in addition to or in place of protons, neutrons, and electrons, such as hyperons or muons. Examples include pionium (
π
 
π+
) and quarkonium atoms.

Leptonic atoms

Leptonic atoms, named using -onium, are exotic atoms constituted by the bound state of a lepton and an antilepton. Examples of such atoms include positronium (
e
 
e+
), muonium (
e
 
μ+
), and "true muonium" (
μ
 
μ+
). Of these positronium and muonium have been experimentally observed, while "true muonium" remains only theoretical.

Molecules

Molecules are the smallest particles into which a substance can be divided while maintaining the chemical properties of the substance. Each type of molecule corresponds to a specific chemical substance. A molecule is a composite of two or more atoms. Atoms are combined in a fixed proportion to form a molecule. Molecule is one of the most basic units of matter.

Ions

Ions are charged atoms (monatomic ions) or molecules (polyatomic ions). They include cations which have a net positive charge, and anions which have a net negative charge.

Quasiparticles

Quasiparticles are effective particles that exist in many particle systems. The field equations of condensed matter physics are remarkably similar to those of high energy particle physics. As a result, much of the theory of particle physics applies to condensed matter physics as well; in particular, there are a selection of field excitations, called quasi-particles, that can be created and explored. These include:

  • Anyons are a generalization of fermions and bosons in two-dimensional systems like sheets of graphene that obeys braid statistics.
  • Dislons are localized collective excitations of a crystal dislocation around the static displacement.
  • Excitons are bound states of an electron and a hole.
  • Hopfions are topological solitons which are the 3D counterpart of the skyrmion.
  • Magnons are coherent excitations of electron spins in a material.
  • Phonons are vibrational modes in a crystal lattice.
  • Plasmons are coherent excitations of a plasma.
  • Plektons are theoretical kind of particle discussed as a generalization of the braid statistics of the anyon to more than two dimensions.
  • Polaritons are mixtures of photons with other quasi-particles.
  • Polarons are moving, charged (quasi-) particles that are surrounded by ions in a material.
  • Skyrmions are a topological solution of the pion field, used to model the low-energy properties of the nucleon, such as the axial vector current coupling and the mass.

Dark matter candidates

The following categories are not unique or distinct: For example, either a WIMP or a WISP is also a FIP.

  • A WIMP (weakly interacting massive particle) is any one of a number of particles that might explain dark matter (such as the neutralino or the sterile neutrino)
  • A WISP (weakly interacting slender particle) is any one of a number of low mass particles that might explain dark matter (such as the axion)
  • A GIMP (gravitationally interacting massive particle) is a particle which provides an alternative explanation of dark matter, instead of the aforementioned WIMP
  • A SIMP (strongly interacting massive particle) is a particle that interact strongly between themselves and weakly with ordinary matter and could form dark matter
  • A SMP (stable massive particle) is a particle that is long-lived and has appreciable mass that could be dark matter
  • A FIP (feebly interacting particle) is a particle that interacts very weakly with conventional matter and could account for dark matter
  • A LSP (lightest supersymmetric particle) is a particle found in supersymmetric models as a contender of WIMPs

Dark energy candidates

Classification by speed

Other

  • Calorons, finite temperature generalization of instantons.
  • Dyons are hypothetical particles with both electric and magnetic charges.
  • Geons are electromagnetic or gravitational waves which are held together in a confined region by the gravitational attraction of their own field of energy.
  • Goldstone bosons are a massless excitation of a field that has been spontaneously broken. The pions are quasi-goldstone bosons (quasi- because they are not exactly massless) of the broken chiral isospin symmetry of quantum chromodynamics.
  • Goldstinos are fermions produced by the spontaneous breaking of supersymmetry; they are the supersymmetric counterpart of Goldstone bosons.
  • Sphalerons are a field configuration which is a saddle point of the Yang–Mills field equations. Sphalerons are used in nonperturbative calculations of non-tunneling rates.
  • Instantons, a field configuration which is a local minimum of the Yang–Mills field equation. Instantons are used in nonperturbative calculations of tunneling rates.
  • Meron, a field configuration which is a non-self-dual solution of the Yang–Mills field equation. The instanton is believed to be composed of two merons.
  • Pomerons, used to explain the elastic scattering of hadrons and the location of Regge poles in Regge theory. A counterpart to odderons.
  • Odderon, a particle composed of a odd number of gluons, detected in 2021. A counterpart to pomerons.
  • Minicharged particle are hypothetical subatomic particles charged with a tiny fraction of the electron charge.
  • Continuous spin particle are hypothetical massless particles related to the classification of the representations of the Poincaré group

Computer-aided software engineering

From Wikipedia, the free encyclopedia ...