Friday, February 28, 2014

BBC News - Will arrest of 'El Chapo' Guzman curb Chicago drugs?

BBC News - Will arrest of 'El Chapo' Guzman curb Chicago drugs?:

"In 2013, the Chicago Crime Commission (CCC) named Guzman the city's Public Enemy Number One, a title previously given only to mob boss Al Capone."

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Thursday, February 27, 2014

[1402.6980] Inflationary schism after Planck2013

[1402.6980] Inflationary schism after Planck2013:

"Classic inflation, the theory described in textbooks, is based on the idea that, beginning from typical initial conditions and assuming a simple inflaton potential with a minimum of fine-tuning, inflation can create exponentially large volumes of space that are generically homogeneous, isotropic and flat, with nearly scale-invariant spectra of density and gravitational wave fluctuations that are adiabatic, Gaussian and have generic predictable properties. In a recent paper, we showed that, in addition to having certain conceptual problems known for decades, classic inflation is for the first time also disfavored by data, specifically the most recent data from WMAP, ACT and Planck2013. Guth, Kaiser and Nomura and Linde have each recently published critiques of our paper, but, as made clear here, we all agree about one thing: the problematic state of classic inflation. Instead, they describe an alternative inflationary paradigm that revises the assumptions and goals of inflation, and perhaps of science generally."

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[1402.6980] Inflationary schism after Planck2013

[1402.6980] Inflationary schism after Planck2013:

"Classic inflation, the theory described in textbooks, is based on the idea that, beginning from typical initial conditions and assuming a simple inflaton potential with a minimum of fine-tuning, inflation can create exponentially large volumes of space that are generically homogeneous, isotropic and flat, with nearly scale-invariant spectra of density and gravitational wave fluctuations that are adiabatic, Gaussian and have generic predictable properties. In a recent paper, we showed that, in addition to having certain conceptual problems known for decades, classic inflation is for the first time also disfavored by data, specifically the most recent data from WMAP, ACT and Planck2013. Guth, Kaiser and Nomura and Linde have each recently published critiques of our paper, but, as made clear here, we all agree about one thing: the problematic state of classic inflation. Instead, they describe an alternative inflationary paradigm that revises the assumptions and goals of inflation, and perhaps of science generally."

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[1402.6686] George Howard Herbig, 1920-2013

[1402.6686] George Howard Herbig, 1920-2013:

 "A great astronomer, George Herbig, passed away in Honolulu on October 12, 2013, at the age of 93. His life and career were long and productive, and consistently dedicated to the careful, thorough research that earned him his reputation. Herbig spent most of his career at Lick Observatory, first as a graduate student, and then from 1949 to 1987 as a staff member, rising through the ranks to Astronomer and becoming Professor as well when the observatory moved to the University of California at Santa Cruz in the late 1960s. Herbig retired from UCSC in 1987 and spent the remainder of his life in Honolulu at the Institute for Astronomy of the University of Hawai`i."

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From Kepler Data, Astronomers Find Galaxy Filled With More but Smaller Worlds -

From Kepler Data, Astronomers Find Galaxy Filled With More but Smaller Worlds -

 "The result is a deluge of small planets that has tipped the cosmic balance from the giant Jupiter-size worlds that were the earliest discovered to smaller, friendlier worlds. “Small planets from the size of Neptune to Earth make up the majority of the planets in the galaxy,” said Douglas Hudgins, exoplanet program scientist at NASA headquarters."

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Wednesday, February 26, 2014

Stephenie Meyer - Wikipedia, the free encyclopedia

Stephenie Meyer - Wikipedia, the free encyclopedia:

"In May 2008, Meyer's adult sci-fi novel The Host, was released by the adult division of Little, Brown and Company. It follows the story of Melanie Stryder and Wanderer, a young woman and an invading alien "soul," who are forced to work as one. The Host debuted at No. 1 on the New York Times Best Seller list[56] and remained on the list for 26 weeks.[57] Meyer has said that she is working on additional books in The Host series and that she intends to write a trilogy, with the second and third books being called "The Soul" and "The Seeker", respectively.[58] In a Q&A session in Kansas City, Meyer stated that she has outlines for the sequels and has done some writing on them, but she has some qualms since The Host universe is a "dangerous place" where characters might die, and she is not sure if she wants to kill them off.[59]"

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Tuesday, February 25, 2014

[1402.5674] Computational Complexity and Black Hole Horizons

[1402.5674] Computational Complexity and Black Hole Horizons:

 "Computational complexity is essential to understanding the properties of black hole horizons. The problem of Alice creating a firewall behind the horizon of Bob's black hole is a problem of computational complexity. In general we find that while creating firewalls is possible, it is extremely difficult and probably impossible for black holes that form in sudden collapse, and then evaporate. On the other hand if the radiation is bottled up then after an exponentially long period of time firewalls may be common. It is possible that gravity will provide tools to study problems of complexity; especially the range of complexity between scrambling and exponential complexity."

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[0902.0169] The Puzzle of Neutron Lifetime

[0902.0169] The Puzzle of Neutron Lifetime:

"In this paper we review the role of the neutron lifetime and discuss the present status of measurements. In view of the large discrepancy observed by the two most precise individual measurements so far we describe the different techniques and point out principle strengths and weaknesses. In particular we discuss the estimation of systematic uncertainties and its correlation to the statistical ones. In order to solve the present puzzle, many new experiments are either ongoing or being proposed. An overview on their possible contribution to this field will be given."

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[physics/0503079] Little Black Holes as Dark Matter Candidates with Feasible Cosmic and Terrestrial Interactions

[physics/0503079] Little Black Holes as Dark Matter Candidates with Feasible Cosmic and Terrestrial Interactions:

Little black holes (LBH) contribute to the accelerated expansion of the Universe, and interact with stars, neutron stars, and planets. A range of proposals are reviewed in which LBH are considered to be a component of dark matter/dark energy. A LBH is a candidate for the 1908 devastation of Tungus Siberia, as important LBH interactions were overlooked. LBH passing through neutron star pulsars are capable of causing a change in. Energy input due to the passage of LBH through the earth, sun, and neutron stars is examined to determine if they could initiate tremors and quakes in such bodies. In encounters with the earth.s atmosphere, LBH can manifest themselves as the core energy source of ball lightning (BL). Relating the LBH incidence rate on earth to BL occurrence has the potential of shedding light on the distribution of LBH in the universe, and their velocities relative to the earth. Most BL features can be explained by a testable LBH model. The total number of degrees of freedom of a d-dimensional body in n-space is derived so that equipartition of energy may be applied in the early universe. Blackbody and Hawking radiation are generalized to n-space. The entropy of LBH and of the universe are examined. The largest possible attractive force, repulsive force, and luminosity in nature are considered in the context of LBH. A question is raised as to whether the Planck scale is truly fundamental. The gravitational fine structure constant is re-examined.

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[1401.3025] Exclusion of the remaining mass window for primordial black holes as the dominant constituent of dark matter

[1401.3025] Exclusion of the remaining mass window for primordial black holes as the dominant constituent of dark matter:

"In a close encounter with a neutron star, a primordial black hole can get gravitationally captured by depositing a considerable amount of energy into nonradial stellar modes. Within a short time, the black hole is trapped inside the star and disrupts it by rapid accretion. We find that the existence of old neutron stars in regions where the dark-matter density rho_{DM}>10^2 sigma/(km/s) GeV/cm^3 (where sigma is the dark-matter velocity dispersion) limits the abundance of primordial black holes in the mass range 10^{17} g < m_{PBH} < 10^{24} g, which was previously unconstrained. In combination with existing limits, our results suggest that primordial black holes cannot be the dominant dark matter constituent."

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[1402.5418] Self-sustained asymmetry of lepton-number emission: A new phenomenon during the supernova shock-accretion phase in three dimensions

[1402.5418] Self-sustained asymmetry of lepton-number emission: A new phenomenon during the supernova shock-accretion phase in three dimensions:

During the stalled-shock phase of our 3D hydrodynamical core-collapse simulations with energy-dependent, 3-flavor neutrino transport, the lepton-number flux (nu_e minus anti-nu_e) emerges predominantly in one hemisphere. This novel, spherical-symmetry breaking neutrino-hydrodynamical instability is termed LESA for "Lepton-number Emission Self-sustained Asymmetry." While the individual nu_e and anti-nu_e fluxes show a pronounced dipole pattern, the heavy-flavor neutrino fluxes and the overall luminosity are almost spherically symmetric. LESA seems to develop stochastically from convective fluctuations, it exists for hundreds of milliseconds or more, and it persists during violent shock sloshing associated with the standing accretion shock instability. The nu_e minus anti-nu_e flux asymmetry originates predominantly below the neutrinosphere in a region of pronounced proto-neutron star (PNS) convection, which is stronger in the hemisphere of enhanced lepton-number flux. On this side of the PNS, the mass-accretion rate of lepton-rich matter is larger, amplifying the lepton-emission asymmetry, because the spherical stellar infall deflects on a dipolar deformation of the stalled shock. This deformation persists despite extremely nonstationary convective overturn behind the shock. The increased shock radius in the hemisphere of less mass accretion and minimal lepton-number flux (anti-nu_e flux maximum) is sustained by stronger convection on this side, which is boosted by stronger neutrino heating because the average anti-nu_e energy is higher than the average nu_e energy. While these different elements of the LESA phenomenon form a consistent picture, a full understanding remains elusive at present. There may be important implications for neutrino-flavor oscillations, the neutron-to-proton ratio in the neutrino-heated supernova ejecta, and neutron-star kicks, which remain to be explored.

We here report the discovery of a new type of low-mode nonradial instability, LESA, which we have observed in 3D hydrodynamical simulations with detailed, energy-dependent, three-flavor neutrino transport using the Prometheus-Vertex code

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[astro-ph/0701358] Dark Matter in an n-Space Expanding Universe

[astro-ph/0701358] Dark Matter in an n-Space Expanding Universe:

"The total number of degrees of freedom of a d-dimensional body in n-space is derived so that equipartition of energy may be applied to a possibly n-dimensional early universe. A comparison is made of a range of proposals to include free and bound black holes as either a small component or the dominant constituent of dark matter in the universe. The hypothesis that dark matter consists in part of atomic gravitationally bound primordial black holes is closely examined in 3-space, as well as in n-space; and the Chavda and Chavda holeum hypothesis is found to be flawed. Blackbody and Hawking radiation are generalized to n-space, and Hawking radiation is shown to be simply proportional to the black hole density. The importance of quantum gravity in understanding the role of early universe dark matter is undermined because present approaches to a theory of quantum gravity violate the equivalence principle. A general heuristic proof for geodesics on an expanding hypersphere is presented. Classical limits of Einstein's General Relativity are considered. A novel approach to the accelerated expansion of the universe is discussed. An anomalous surprising aspect of 4-space is demonstrated."

This assumes negligible Hawking radiation

As 95% of the mass of the universe, LBH essentially hold the universe together gravitationally, and their directed radiation contributes to its accelerated expansion. That many LBH doing Hawking Radiation would fry the universe. Unlike LBH that Hawking radiate, my LBH are long-lived because in my model of Gravitational Tunneling Radiation (GTR) they radiate much, much less and the radiation is beamed

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The Five Ages of the Universe - Wikipedia, the free encyclopedia

The Five Ages of the Universe - Wikipedia, the free encyclopedia:

"Stelliferous Era[edit]
The Stelliferous Era is defined as "6 < n < 14". This is the current era, in which matter is arranged in the form of stars, galaxies, and galaxy clusters, and most energy is produced in stars. Massive stars use up their fuel very rapidly, in as little as a few million years. Eventually, the only stars remaining will be miserly red dwarf stars. By the end of this era, bright stars as we know them will be gone, their nuclear fuel exhausted, and only white dwarfs, brown dwarfs, and black holes will remain. In this section, Olbers' paradox is discussed."

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The Five Ages of the Universe - Wikipedia, the free encyclopedia

The Five Ages of the Universe - Wikipedia, the free encyclopedia:

"The book The Five Ages of the Universe discusses the history, present state, and probable future of the universe, according to cosmologists' current understanding. The book divides the timeline of the universe into five eras: the primordial Era, the Stelliferous Era, the Degenerate Era, the Black Hole Era and the Dark Era."

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Monday, February 24, 2014

A variant of the Titius-Bode Law

A variant of the Titius-Bode Law:

"The study of the geometric distribution of the planets invariably mentions the Titius Bode law as an attempt to classify their heliocentric distances through a succession of integer numbers. With the discovery of more planetary objects better support is given to the basic principle of the law through their orbital parameters. We briefly refer to a classification of orbital parameters using Kepler's proportionality parameter and discuss the problem of applying the TB Law to extrasolar systems. We also review work by various authors who have proposed functions which reproduce with some degree of certainty the planetary heliocentric distances, and we compare them to our variant of the Titius-Bode Law."

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e^(.6122x-2.8176) - Wolfram|Alpha

e^(.6122x-2.8176) - Wolfram|Alpha:

Generalized Titius-Bode Law

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G.P. Gladyshev

Physicochemical processes taking place in space are characterized by a number of specific features that distinguish them from conditions in the terrestrial atmosphere. They are generally effected in ultrahigh vacuum at extremal temperatures in ultrastrong or ultraweak fields (electrical, magnetic, or gravitational). The range of problems pertaining to the chemical evolution of matter in space is extremely broad [1-6], and it is impossible to discuss more than a small portion of them in a single paper. The present article is devoted to individual aspects of the course of chemical processes under the extremal conditions that might have obtained during formation of the Solar System and other planetary systems. Particular attention will be given to problems of the spatially periodic condensation of matter under the conditions of the protosolar system, which bad not previously been taken into account by evolutionary theories.
We will follow the published general schema of the processes involved [1] and consider the stages in the evolution of the Solar System. The first stage was the development of the Protosun, which was formed as a result of accretion from the original Solar System cloud; the second was disposition of the gas and dust forming the atmosphere in the vicinity of the magnetized central body, the third was transfer of momentum from the Protosun to the surrounding atmosphere, so that the gas and dust particles began to move in Keplerian orbits relative to the Sun. The decisive role during these stages was played by magnetohydrodynamic effects, since the gas falling toward the sun was quite rarified and constituted a plasma. As the matter became concentrated around the Sun, the density of the cloud increased and the influence of magnetohydrodynamic effects diminished. When the protocloud coalesced and became a disk, these effects became small. The stages described above were completed relatively rapidly, within 107-108years.
According to the theory elaborated in [7-13], there then ensued a protracted fourth evolutionary stage, formation of the primary Solar System rings, which ended relatively recently. It was associated with diffusion (mass transfer) of the solar material to the evolving disk, in which spatially periodic condensation of material from the supersaturated state took place to form rings of condensed matter (the latter subsequently accumulated into the planets as system development progressed). It was shown in these studies that the matter concentration in the protoclouds could have remained quite high for some time, so that the role of the magnetohydrodynamic effects discussed in monograph [1] would not have been as substantial in the stage under consideration. The decisive role was apparently played by diffusion of material from the central bodies into the corresponding protoclouds and chemical reactions leading to condensation from the supersaturated state. It can be assumed with some measure of approximation that Ficke's law:

is satisfied starting at some distance rn' from the surface of the Protosun, where the are the average concentrations of material diffusing from the central body S and cloud material N, while DS,N is the average diffusion coefficient. An expression relating the location (rn) of the n-th ring and the time of its formation (tn) is easily obtained from (1):

Liesegang's theory of periodic condensation can be used to explain the empirical Titius-Bode rule of planetary distances, according to which the distance of the n-th planet from the Sun (rn) satisfies the relation [4]:
Table I
Some Planetary Parameters [1] and Characteristic Durations of Stages in Evolution of Solar System

Planetary mass, m0·10-27, g

Major semiaxis, r·10-13, cm

Planetary radius, Rm·10-9, cm

Formation time of primary ring, tp.r·10-6, years

Planetary age, t·10-9, cm

Jet formation time tj, years

Planetary nucleus formation time, tp.n·10-6,years

Accretion time, tac·10-6, years





























































1.4· 103

>104 **

8.8· 103





2.25· 103


2.3· 103

>104 **

>104 **

Pluto *




3.9· 103


3.0· 103


*Calculations made for regular planet in far reaches of Pluto's orbit. **Characteristic times tac and tp.nfor outer planets are comparatively long, since flattening of torus was not taken into account in this approximation.

where rn, is the greater semiaxis of the orbit of the n-th planet and r, and r0 are empirical constants.
After specifying physically reasonable values for the parameters [1,14], we can obtain the values of tnfrom expression (2), i.e., estimate the times at which the primary rings were formed (tnє tp.r):

where m and V are the mass and volume of the protoplanetary disk,s and M are the average diameter and molecular mass of the diffusing particles, g is a constant (g =6), T is the absolute temperature, and R is the universal gas constant.
The results of these estimates are given in Table 1. The age of a planet is estimated as the difference between the total age of the Solar System (assumed to be ~ 4.5• 10-9 years) and the corresponding tp.r. According to the concepts elaborated here, the further a planet is located from the Sun, the younger it is. The theory predicts the existence of ring systems and satellites in an active evolutionary stage for young planets.
As the primary rings initially formed near the Sun developed, the next stage of evolution proceeded. A ring of condensed matter was formed in the jets, consisting of solid grains and gas. The accretive evolution of the jets of each protoplanetary ring led to development of a planetesimal and then of a planetary core, consisting basically of compounds of heavy elements. During formation of large planets, gravitational capture of uncondensed substances (H2, He, etc.) occurred when the core reached sufficient size. As the planetary cores grew and a magnetic field appeared, magnetohydrodynamic effects became perceptible in their initial protosatellite clouds. As in the case of the Sun, gas and dust were distributed around each planet, forming an protodoud; transfer of momentum occurred, and the cloud particles began to move in Keplerian orbits. As concentration of the material progressed, the magnetohydrodynamic effects became weaker again. Gravitational compression led to warming of the protoplanet and to ejection (diffusion) of its material into the gas "shells" of the protocloud, which was apparently accompanied by spatially periodic condensation and formation of the primary rings of regular protosatellites and then of planetary satellites. The fourth and final evolutionary stages proceeded in parallel.
Thus, the general premises of the magnetohydrodynamic theory of Solar System evolution [1] are in good qualitative agreement with the theory of spatially periodic condensation. Quantitative assessment of the electromagnetic effects [7] shows that their role might actually have diminished as the protodisks developed and constricted and again increased in those regions where matter condensed and the gases became incandescent. The criterion in gas dynamics that justifies neglecting electromagnetic effects is the characteristic magnetohydrodynamic parameter L, which should, according to [1], be far less than one:

where B is the magnetic induction, l is the linear extent of the medium, sE is the medium electrical conductivity, PB is the magnetic permeability, r is the medium density, and c is the speed of light.
We know that L>>1 and usually equals 1015—1020 for a number of stellar and interplanetary regions. In the E layer of planetary ionosphere, L~1; for planetary atmospheres and hydrospheres, L<<1. It is thought [1] that LЈ 106 in the interior of cold dark clouds.
The parameter L was estimated for the central regions of forming protodisks in [7], proceeding from the average parameters of the solar disk and utilizing data on the planetary atmospheres of the Earth and Mars. Assuming that the inner layers of the disk must be screened from ionizing-radiation by a layer of material h<1, r2 (where r1 and r2 are the radius and average thickness of the disk) in order for criterion (5) to be satisfied, it was shown that this condition is fulfilled not only in the case of Earth and Mars but also over the series comprising the Solar System and the satellite systems of Jupiter, Saturn, Uranus, and Neptune (and more strictly so on moving toward the outer planets).
The final stage in protoplanet formation is gas capture by the jets, or planetary nuclei. The basic mechanism of the process is treated by utilizing the model of gas molecule 'adhesion' to a cold solid surface [1]. Moreover, according to [7], gas apparently accumulates as a result of 'apparent attraction,' i.e., multiple collisions of gas molecules with jet grains. Some of the gas is not retained by the jet and diffuses out of it, forming a jet atmosphere. If we assume the rate at which gas mass is absorbed (dm/dt) to be proportional to the nucleus surface area (A) and the gas mass (m) in the volume from which diffusion takes place, i.e.,

where g ' is a proportionality factor, we find that, when A=const, the loss of gas cloud mass as a result of gas absorption by jet particles is described by the relation:

When A varies (for gas absorption by a planetary nucleus), we have in the general case:

where R0 and M are the initial size and mass of the nucleus, q is the density of the nucleus, r is the density of the growing layer during gas condensation, nig is the gas cloud mass at the starting time, and m is the cloud gas mass at time t.
Equation (7) and the solution of Eq. (8) can be used to calculate the times tj, and tp.n, which characterize the decrease in gas mass (e.g., by a factor of 10) during formation of a jet and planetary nucleus respectively. The results of such estimates are given in Table 1. The accretion times tac are also listed, for purposes of comparison [1]. It can be seen that tp.n differs from tac by a factor of 2-10 and that tj<<tp.ntac. It can thus be assumed in first approximation that the limiting stages of the formation of large planets in the Solar System is diffusion, which leads to condensation of material from the supersaturated state and formation of primary rings, as well as hydrogen and helium accretion by planetary nuclei.
Periodic condensation should inevitably be detected in the deep atmospheric layers of planets, comets, and other bodies; the process in cometary atmospheres can serve as a model of the condensation that occurred during formation of the Solar System. There is reason to believe [15-17] that L<<1 and that magnetohydrodynamic effects are not decisive in the inner atmospheric layers of comets that are not very close to the sun and extend for several thousand kilometers. Cometary nuclei generally contain a number of comparatively volatile compounds, such as H2O, CO2, CO, HCN, etc. As comets approach the Sun, these substances begin to evaporate at high rates [15,16]. The vapor tension of substances at the surface of the nucleus is approximately equal to the equilibrium value defined by the Clausius-Clapeyron equation:
Table 2
Known Interstellar Molecules and Ions [22]
Consisting solely of C and H
Containing O
Containing N
Containing O and N
Containing S and Si
Cє C
(Cє C)2H
H3C(Cє C)2H
H(Cє C)2CN
H(Cє C)3CN
H(Cє C)4CN
H(Cє C)5CN
H3C(Cє C)2CN

Fig. 1. Photograph of regular spatially periodic condensation of NH4Cl. Annular deposit structures produced during two-dimensional diffusion of NH3 in HCl vapor.

where p and T with appropriate indices are the initial and final equilibrium pressure and temperature, and ; DH is the change in enthalpy on sublunation and R is the universal gas constant.
Rapid sublimation of material begins at some distance from the Sun, and it then expands adiabatically. Adiabatic expansion is accompanied by cooling of the gas; the latter is supercooled in this case. Published relations for the adiabatic process were used in [7] to estimate the characteristic dimensions of the material condensation zones:
where Vad is the volume and is the heat capacity ratio.
If one solves Eqs. (9) and (10) jointly and specifies the supersaturation , one can estimate the ratio r2/r1 where r1 and r2, are the radii of successive zones of spherical (annular, etc.) structure formation. The process by which successive condensation zones are formed can be repeated so long as turbulent magnetohydrodynamic effects do not disturb the structure. It has been shown, for example, that only one or two condensed CO2 structures can be formed for s = 40 in a cometary atmosphere. Periodic structures consisting of H20 ice fogs can be formed in cometary atmospheres near the sun. The values of s for water in cometary atmospheres should apparently vary over the range 1-5, and instances in which several condensation zones develop are therefore possible. Comet Donati provides an example supporting the approximate model under consideration [15]. The comet put out five envelopes over the period covering 4 and 5 October 1858. Then-formation mechanism did not preclude condensation of material from the supersaturated state. The model under discussion can in principle be validated by putting artificial comets containing volatile components into earth orbits.
Figure I is a photograph of a system of periodic NH4Cl deposits produced (according to the data of (18]) during two-dimensional diffusion of NH3 in HCl vapor. The pattern depicted in this figure does not differ in its fundamentals from the phenomenon that should be observed on a large scale during formation of planetary and satellite systems, since there is no reason to believe that the classical mass transfer laws and concepts of condensation from the supersaturated state established under terrestrial conditions (12,19-21] are not satisfied over long time cycles and vast distances.
We will now turn to probable models of the chemical transformations that occur in different stages of planetary system formation. There can be many such models, since conditions for formation of such systems differ substantially in different parts of the universe. One illustration of the foregoing is the great variety of interstellar molecules that have now been detected and are present under different conditions in different systems. Thus, besides H2, He, and other inert gases, diffuse clouds, cold dense clouds, and stellar envelopes have been found to contain about 70 molecular and ionic species, extending through atomic number 13 [3,22,28] (see. e.g., Table 2). It should also be remarked that, as is well known, various hydrocarbons (CH4, C2H2, C2H6, etc.) have been detected in the planetary atmospheres of the Solar System, together with H2, He, NH3, PH3, CO, CO2, H2O, HCN, and so forth. The present survey will not attempt to cover all the multiplicity of chemical processes that occurred in material condensation during the early stages of formation of the Solar System [3 -5,23-28]. We will merely touch upon those reactions that probably could have been responsible for transport of heavy elements from the central Solar System to the periphery and formation of rings of condensed matter, followed by planets.
According to the theory being discussed here, appearance of primary rings is a consequence of chemical reaction of the substances in the cloud (N) and those from the central body (S) that diffuse into the cloud surrounding the planet. One necessary condition for condensation is supersaturation. This planetary formation mechanism should apparently bold for stars embedded in dark nebulae and going through the T body stage (there is reason to suppose that our Sun went through this stage at some point). It is not at all necessary for periodic condensation that the chemical composition of the central body gas phase and cloud differ: periodic condensation can also take place when there is a temperature gradient in the cloud. However, it is difficult to conceive of a case in which the compositions of the protostar gas envelope and cloud would be identical Thus, if we assume that stars of the Sun's type are formed as a result of gravitational compression of interstellar clouds, then gravitational separation of elements is possible during the collapse. The star formed can contain more heavy elements than the-surrounding cloud. In addition, the occurrence of nuclear reactions in stars can cause their composition to differ significantly from that of the clouds around them. As a consequence of the low cloud temperature, most of the heavy elements in the cloud can be in solid (dust) form even when the central body and cloud have the same overall composition.
As was noted above, many reported dense clouds contain such molecules as H2, He, CO, HCN, NH3, H2O, H2CO, SiO, H2S, etc., as well as a variety of ions and radicals; the principal cloud components are often H2, He, CO, and H2O. The CO concentration is far lower than the H2 or He concentration, but it is, as a rule, relatively high in comparison with that of other components. It can therefore be supposed that H2 and CO (or H2, CO, and H2O) play the major role in reactions. The H2 and CO in a cloud can be responsible for transporting virtually all heavy elements to the peripheral regions of a planetary system, in the form of hydrides and carbonyls. Elements emanating from a protostar react with one another in its vicinity to form volatile molecules [e.g., H2, CO, SiO, FeH, CH, SiH, FeHx(CO)y, etc.], which diffuse into the cloud. As diffusion proceeds in low-temperature zones, these molecules can react with the cloud material and be converted to new volatile particles, which diffuse further. Individual molecules that are thermodynamically stable under given conditions may not enter into further reactions with the cloud matter and, after attaining "supersaturation", condense to form primary rings. Diffusion of protostar material as a result of tandem transport reactions can thus be accompanied by a change in its nature. Despite the formation of various substances that are apparently characterized by different diffusion and supersaturation coefficients, the Titius-Bode rule is relatively well satisfied. This can probably be attributed to the fact that formation of primary rings is due primarily to reactions of several of the most common elements in the universe, e.g., Fe, Mg, S, Si, O, N, C, and H [23 -29] (see Table 3), to the fact that the change in the nature of the condensed material can be neglected, and to the fact that condensation zones with greater mass "absorb" small zones as they undergo conversion to planets (satellites).
Table 3
Abundance of Elements in the Cosmos
Relative abundance (by number of atoms)
3.75· 10-4
8.7· 10-5
4.4· 10-4
2.6· 10-5
3.2· 10-5
1.4· 10-5
3.2· 10-5
It thus seems sensible to suppose that the basic initial processes might be formation of volatile hydrides, carbonyls, and carbonyl hydrides of iron- and magnesium-group elements, such as FeH and FeHn, (CO)m, type, together with carbonyl halohydrides and carbonyl halides of the Fe(CO)mF and Fe(CO)mCl type and compounds of the FeHn(CO)m(SiO)pHalr type, where the sum of n, m, p, and r can vary from 1 to 5. Formation of these substances is accompanied by evolution of heat (i.e., their synthesis at the low temperatures observed in the neighborhood of the Sun and in clouds is thermodynamically advantageous) and are stable in a hydrogen atmosphere. The same assumption can be made regarding similar compounds of other heavy elements (Cu, Ag, Au, Ca, Zn, Hg, etc.). If the concentrations of H, C, and Si in a cloud are sufficiently high, these compounds do not interact with O, since they react primarily with C, Si and H to form CO, SiO, OH(H2O), etc..
If the H2O content in a cloud is elevated (for example, it is believed [27,49] that H2O can be formed in space from H2 and CO by reactions of the Fisher-Tropsch type, nCO + (n + m/2)H2 ® CnHm + nH2O, which take place at high temperatures at catalysts, i.e., magnetite and hydrated silicates), then the compounds being transported can react with the water molecules to produce substances capable of condensing from the supersaturated state. If the cloud has a CO content higher than that in the protostar atmosphere and contains little H2O, then volatile hydrides, carbonyl hydrides, and carbonyl halohydrides of the FeH, FeHn(CO)m and Fe(CO)mHal types formed in the neighborhood of the protostar are converted to comparatively low-volatility carbonyls of the Fe(CO)mSiO type, which are capable for forming condensation zones. In clouds containing high concentrations of NO, NH3 and SiO, hydrides and carbonyl hydrides can be converted to compounds such as Fe(CO)3NO, Fe(CO)3NH3, FeH(CO)mSiO, etc. The model is thus applicable not only to actual cases where H2, CO, and H2O molecules predominate in the cloud, but also to hypothetical cases, when there is an excess of NH3 or NO molecules.
The model of heavy element transport that presumes formation of hydrides and carbonyl hydrides agrees with our conceptions of the composition of planetary and satellite cores. For example, reaction of compounds of the FeHn(CO)mSiO type with water leads to silicate formation. Moreover, after such substances condense and accumulate in solid form, they are converted to iron, silicates, and CO as a result of even slight warming. The hypothesis that metal carbonyls have played a substantial part in the chemical evolution of the Solar System [10] is supported by the results of [30] and [31], where one model of Triton was developed. The author of the latter study showed that this satellite of Neptune may consist of Fe2(CO)9 (91%) and CH4 (9%). It should be noted that one significant fact supporting the model under consideration for formation of the Solar System and other planetary systems is the existence of SNC meteorites, whose age is only 109 years.
The reactions of ions formed under the action of cosmic rays play an essential role in periodic condensation in cold dense clouds consisting basically of H2 He, CO, and SiO, since these are exothermal reactions with low activation energy [22,28]. If we assume the composition of the protostar to differ from that of the protocloud primarily in the amount of He (which is formed in the protostar as hydrogen is burned), this can lead to various reactions. Since the He+ ions formed under the action of cosmic rays (He + cosmic ray protons ® He+ + e- + protons') react slowly with H2, they are present in significant amounts in the cloud. As it has a strong affinity for electrons, He+ is capable of reacting with neutral particles, e.g. [22,29,32]:
He++CO® C++O+He
He++O2® O++O+He
He++N2® N++N+He
He++CN® C++N+He
He++N2® N2++He
He++SiO® Si++O+He
The active C+ and O particles formed can react with the cloud components to produce condensed compounds.
The general mechanisms of spatially periodic condensation can in principle extend to formation of galaxies, assuming that hydrogen and helium synthesis is possible not only in stars, but also from the "supersaturated" state in outer space by reactions of the type [13]:
We cannot preclude the possibility that the following reactions of gaseous compounds also played an important role under terrestrial conditions:
SiH4+2H2O® SiO2Ї +4H2
SiF4+2H2O® SiO2Ї +4HF
SiCl4+2H2O® SiO2Ї +4HCl
AlCl6+3H2O® Al2O3Ї +6HCl
Fe(CO)5+O2® Fe2O3Ї , CO, CO2
There is thus reason to believe that the cores of all the protoplanets in the Solar System (and certain other planetary systems) consist of metal/silicate material. If we assume typical temperatures in the perisolar disk to be in the range 100-200 K at a distance of 1 AU and 10-20K at a distance of 10 AU, we can draw the following conclusion [33]: compounds of metals and silicon condense in the regions of space where the terrestrial-group planets are located, while all substances except hydrogen and helium condense in the regions occupied by the outer planets. The hydrogen and helium subsequently undergo gravitational capture, mostly by the Jupiter-group planets. Gravitational warming of the planets, which leads to development of satellite systems, as in the case of the Sun, later promotes changes in protoplanet chemical composition.
The model of the physicochemical processes that have played a significant role at definite stages in the evolution of the Solar System considered here is undoubtedly oversimplified. Nevertheless, it makes it possible to determine the age of the planets and account for the Titius-Bode rule. According to our theories, the further a planet is from the sun, the younger it is. The model in question made it possible to predict the existence of rings in the satellite systems of young planets (Uranus, Neptune, and Jupiter) long before they were discovered, as well as individual features of the rings and satellite systems of Uranus, Neptune, and Triton that have been confirmed by data obtained with spacecraft [7].
Another interesting aspect of the evolution of chemicals in space is related to the development of chirality (optical activity). One important feature of chemical reactions in ultrararefied molecular protoclouds in space is the far stronger dependence of reaction mechanism on the presence of force fields (electrical, magnetic, and gravitational) than is the case under the conditions of the terrestrial lithosphere, which can promote formation of excesses of optically active substances having a definite orientation. We cannot preclude the possibility that optically active substances might have been generated during formation of the Solar System.
The optical activity of substances of biological origin is an inseparable property of life and is due to inclusion in biomolecules of only amino acid L-isomers and sugar D-isomers (or fragments). Many theories have been advanced to explain this phenomenon [34-47]. Evolutionary concepts assume gradual deracemization under the influence of some asymmetric advantage factor promoting accumulation of one isomer. The concept of spontaneous deracemization was advanced comparatively recently [43,44] and holds that chiral purity arose as a result of a spontaneous transition to the prebiological (chemical) stage of evolution. Spontaneous racemization subsequently occurred in inorganic nature, while chirality persisted in living organisms as a consequence of self-replication and survived as a memory of the state of the environment during the birth of life on Earth. It has been shown that polynucleotide self-replication can occur only in a chirally pure medium [45,46]. It has been hypothesized that life originates in cold dense interstellar clouds [47,48]. The effect of various asymmetric agents, including natural physical fields, radiations, and combinations thereof, and nonconservation of parity in weak interactions, has been discussed. It was shown in. [7,10] that the stereospecific action of such fields can be manifested to a far greater extent in ultrararified molecular clouds than under terrestrial conditions, since the energy of atomic and molecular thermal motion at ordinary temperatures (t ~ 300 K) is far greater than that of the orienting effect of natural asymmetric fields. Thus, the interaction with the relict radiation having a temperature T0=2.7K becomes decisive in dark clouds (the kinetic temperature characteristic of interstellar clouds can be quite high, Tk=100-200K). The low-temperature residual radiation is sometimes not capable of 'masking' the stereospecific action of sufficiently strong asymmetric fields.
The occupancy of molecular energy levels in ultrararified gases, where the pressure is extremely low, does not follow Boltzmann's law:

where nu and nl are the concentrations of molecules in the upper and lower levels of a given transition respectively, gu and gl are the statistical weights of the levels, n 0 is the transition frequency, h and k are the Planck and Boltzmann constants respectively, and Ts is the excitation temperature, which equals the kinetic temperature Tk of the ambient medium under conditions of thermodynamic equilibrium for all levels.
These deviations from local thermodynamic equilibrium are due to low medium density, with collision frequency being very small in comparison with the rate of spontaneous transitions. This causes the higher energy levels to be underpopulated. Moreover, conditions such that molecules react with one another not only in the electronic and vibrational ground states but even in rotational states are created in interstellar clouds [49].
According to the calculations made in [7], the Earth's magnetic field can have a perceptible effect only on nonrotating molecules. The proportion of nonrotating molecules oriented by the Earth's magnetic field is determined by the expression

where n(l) and n(2) are the concentrations of molecules oriented parallel and perpendicular to the field respectively, n is the total molecular concentration. A, B, and C are the molecular rotational constants, s ' is the number of physically indistinguishable molecular orientations, W is the orientation energy of a paramagnetic molecule in the Earth's field, and T is the molecular excitation temperature.
If we substitute T=300K into (12), we obtain [n(l)-n(2)]/n@ 10-9, so that the molecules are almost randomly oriented. When , the orientation becomes quite perceptible. A graphic example of the formation of optically active RCH(OH)CN molecules is the process
which can occur in space.
Similar reactions in which L- or D-forms are generated can in principle take place not only when the reactant partides are oriented in collisions in the gaseous state, but also when one of the reactants is absorbed on an oriented solid particle and the other is in the gas phase. Moreover, interaction of two appropriate molecules adsorbed on oriented solid particles is possible in rarified clouds. However, the relative role of these mechanisms in the evolution of matter is unclear from the standpoint of the chirality problem. Neither can we overlook the influence exerted by electromagnetic fields in combination with the gravitational fields of sufficiently massive oriented structures on selection or differentiation of chemical substances during the course of evolution [7,50].
1. H.Alfven and G.Arrhenius, Evolution of the Solar System [Russian translation], Mir, Moscow, 1979.
2. V.S.Safronov and A.V.Vitjazev, in: Chemistry and Physics of Terrestrial Planets, Springer-Verlag, N.Y., Berlin, Heidelberg, 1986, pp. 1-29.
3. B.E.Turner and L.M.Zurus, in: Galactic and Extragalactic Radio Astronomy, Springer-Verlag, Berlin, Heidelberg, N.Y., 1988, pp. 200-254.
4. H.Reeves (Editor), Origin of the Solar System [Russian translation], Mir, Moscow, 1976.
5. A.G.W.Cameron, Space Sd. Revs., vol. 15, no. 1, pp. 121-146, 1973.
6. L.Grossman and J.W.Larimer, Rev.Geophys. Space Phys., vol. 12, no. I, pp. 71-101, 1974.
7. G.P.Gladyshev, Thermodynamics and Macrokinetics of Natural Hierarchic Processes [in Russian], Nauka, Moscow, 1988.
8. G.P.Gladyshev, The Role of Physicochemical Processes in Formation of Planetary Systems [in Russian], IKhF AN SSSR, Chernogolovka, 1977.
9. G.P.Gladyshev, Moon and Planets, vol. 18, no. 2, pp. 217-221, 1978.
10. G.P.Gladyshev, Ibid., vol. 19, no. I, pp. 89-98.
11. V.P.Budtov and G. P. Gladyshev, Ibid., vol. 20, no. 3, pp. 213-218, 1979.
12. G.P.Gladyshev and V. P. Budtov, Ibid., voL 25, no. 4, pp. 413-425, 1981.
13. G.P.Gladyshev, Condensation of Matter in the Universe [in Russian], Bash. fit AN SSSR, Ufa, 1982.
14. J.Hirschfelder, C.Curtis, and R.Byrd, Molecular Theory of Gases and Liquids [Russian translation], Mir, Moscow, 1961.
15. F.L.Whipple, in: Comets and the Origin of Life [Russian translation], Mir, Moscow, 1984, pp. 9—28.
16. See [15], pp. 96-108.
17. A.V.Kolesnichenko and M. Ya. Marov, Modeling Fluid-Dynamic Processes in Gaseous Comet Atmospheres [in Russian], In-t priki. matematiki AN SSSR, Moscow, 1985.
18. V.N.Gorshenev and G. P. Gladyshev, Zh. fiz. khirnii, voL 55, no. II, pp. 2897-2903, 1981.
19. R.R.Rogers, Short Course in Cloud Physics [Russian translation], Gidrometeoizdat, Leningrad, 1979.
20. A.M.Borovikov, I.I.Gaivoronskii, E. G. Zak, et al„ Cloud Physics [m Russian], Gidrometeoizdat, Leningrad, 1961.
21. A.G.Amelin, Theoretical Principles of Nebula Formation [in Russian], Khimiya, Moscow, 1972.
22. D.Smith, Phil. Trans. Roy. Soc. London A, voL 323, no. 1572, pp. 269-286, 1987.
23. J.S.Lewis, Icarus, vol. 16, no. 2, pp. 241-253, 1972.
24. J.S.Lewis, Annu. Rev. Phys. Chem., vol. 24, pp. 339-351, 1973.
25. S.K.Saxena and G. Eriksson, see [2], pp. 30-105.
26. G.V.Voitkevich, Problems in Cosmochemistry [in Russian], lzd-vo Rost. u-ta, Rostov, 1987.
27. G.V.Voitkevich, Foundations of a Theory of the Origin of Earth [in Russian], Nedra, Moscow, 1988.
28. H.E.Suess, Chemistry of the Solar System: an Elementary Introduction to Cosmochemistry, Wiley, N.Y., 1987.
29. E.Herbst and W.Klemperer, Astrophys. J„ vol. 185, pp. 505-533, 1973.
30. G.H.A.Cole, Geophys. J. Roy. Soc. Astron. Soc., vol. 77, pp. 549-557, 1984.
31. V.Celebonovic, Earth, Moon and Planets, vol. 34, no. I, pp. 59-63, 1984.
32. J.L.Turner and A.Dalgarno, Astrophys. J„ vol. 213, pp. 386-389, 1977.
33. See [4], pp. 107-115.
34.I.Idsumi and A.Tai, Stereodifferentiating Reactions [Russian translation], Mir, Moscow, 1979.
35. M.Calvin, Chemical Evolution [Russian translation], Mir, Moscow, 1971.
36. M.Rutten, Origin of Life [Russian translation], Mir, Moscow, 1973.
37. S.Fox and K.Dose, Molecular Evolution and the Origins of Life [Russian translation], Mir, Moscow,
38. E.Broda, Evolution of Bioenergetic Processes [Russian translation], Mir, Moscow, 1978.
39. W.Thiemann, Naturwissenshaften, voL 61, pp. 476-483, 1974.
40. W.Thiemann. Orig. Life, voL II, no. I, pp. 187-190, 1981.
41. W.L.Keszthelyi, Ibid., p. 191.
42. V.A.Kizel, Physical Factors Responsible for Dissymmetry in Living Systems [in Russian], Nauka, Moscow, 1985.
43. L.L.Morozov, Orig. Life, voL 9, no. 3, pp. 187-217, 1979.
44. V.I.Gol'danskii and V.V.Kuz'min, Uspekhi fiz. nauk, voL 157, no. I, pp. 3-50, 1989.
45. V.A.Avetisov, S.A.Anikin, V.I.Gol'danskii, and V.V.Kuz'min, DokLAN SSSR, voL 282, no. I, pp.184-186,1985.
46. V.I.Gol'danskii, V.A.Avetisov, and V.V.Kuz'min, Ibid., vol. 190, no. 3, pp. 734-738, 1986.
47. F.Hoyle and N.C.Wickramasinghe, Lifedoud. The Origin of Life in the Universe, J. M. Dent and Sons LTD, London, Toronto, Melbourne, 1978.
48. V.I.Gol'danskii, Nature, voL 279, no. 5709, pp. 109-115, 1979.
49. B.E.Turner, in: Galactic and Extragalactic Radio Astronomy, Springer-Verlag, Berlin, Heidelberg, N.Y., 1974, pp. 303-399.
50. G.P.Gladyshev, Yu.B.Monakov, A.A.Berg, and V.P.Grigor'eva, On Radical Initiator Decay in an Ultracentrifuge Field [in Russian], Bash. filial AN SSSR, Ufa, 1981.
See: chirality

Taken From:  G.P. Gladyshev

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