The Exploded Planet Hypothesis: The Destruction of Tiamat/Electra/Maldek and the Creation of the Asteroid Belt
(1) satellites of asteroids(2) satellites of comets(3) salt water in meteorites(4) “roll marks” leading to boulders on asteroids(5) the time and peak rate of the 1999 Leonid meteor storm(6) explosion signatures for asteroids(7) strongly spiked energy parameter for new comets(8) distribution of black material on slowly rotating airless bodies(9) splitting velocities of comets(10) Mars is a former moon of an exploded planet
In the latter half of the 18th century, when only six major planets were known, interest was attracted to the regularity of the spacing of their orbits from the Sun.
In the 1860s, Simon Newcomb suggested a test to distinguish the two theories of origin of the asteroids.
If they came from an exploded planet, all of them should reach some common distance from the Sun, the distance at which the explosion occurred, somewhere along each orbit. But if asteroids came from the primeval solar nebula, then roughly circular, non-intersecting orbits ought to occur over a wide range of solar distances between Mars and Jupiter.
Newcomb applied the test and determined that several asteroids had non-intersecting orbits. He therefore concluded that the solar nebula hypothesis was the better model. Newcomb’s basic idea was a good one. But only a few dozen asteroids were known at the time, and Newcomb did not anticipate several confounding factors for this test.
He also did not appreciate that planetary perturbations, especially by Jupiter, can change the long-term average eccentricity (degree of circularity) of each asteroid’s orbit. Finally, Newcomb did not consider that more than one planet might have exploded, contributing additional asteroids with some different mean distance. In Newcomb’s time, no evidence existed to justify these complications.
When Newcomb’s test is redone today, the result is that an explosion origin is strongly indicated for main belt asteroids. In fact, the totality of evidence indicates two exploded parent bodies,
- one in the main asteroid belt at the “missing planet” location, and
- one near the present-day orbit of Mars.
Although over 10,000 asteroids have well-determined orbits, the combined mass of all other asteroids is not as great as that of the largest asteroid, Ceres.
Consider what would happen if the Earth exploded today. Surface and crustal rocks would shatter and fragment, but remain rocks. However, rocks from depths greater than about 40 km are under so much pressure at high temperature that, if suddenly released into a vacuum, such rocks would vaporize. As a consequence, over 99% of the Earth’s total mass would vaporize in an explosion, with only its low-pressure crustal and upper mantle layers surviving.The situation worsens for a larger planet, where the interior pressures and temperatures get higher more quickly with depth. In fact, all planets in our solar system more massive than Earth (starting with Uranus at about 15 Earth masses) are gas giants with no solid surfaces, and would be expected to leave no asteroids if they exploded.
Bodies smaller than Earth, such as our Moon, would leave a substantially higher percentage of their mass in asteroids. But the Moon has only about 0.01 of Earth’s mass to begin with.
In short, asteroid belts with masses of order 0.001 Earth masses are the norm when terrestrial-planet-sized bodies explode. Meteorites provide direct evidence for this scenario of rocks either surviving or being vaporized.
Modern Evidence for Exploded Planets
Two important lines of evidence that asteroids originated in an explosion are the explosion signatures (described later in this article), and the rms velocity among asteroids, which is as large as is allowed by the laws of dynamics for stable orbits.
In other words, the asteroid belt is certainly the remnant of a larger population of bodies, many of which gravitationally escaped the solar system or collided with the Sun or planets.
Two important lines of evidence that meteoroids originated in an explosion are:
(1) The most common meteorite type, chondrites, have all been partially melted by exposure to a “rapid heating event”. Other asteroids show exposure to a heavy neutron flux. Blackening and shock are also common traits.(2) The time meteoroids have been traveling in space exposed to cosmic rays is relatively short, typically millions of years. Evidence of multiple exposure-age patterns, as would happen from repeated break-ups, is generally not seen.
Saturn’s moon Iapetus is one such case, because its rotation period is nearly 80 days long. Figure 1 shows a spacecraft image of Iapetus. One side is icy bright; the other is coal black. The difference in albedo is a factor of five. Gray areas are extrapolations of black areas into regions not yet photographed. As such, they represent a prediction of what will be seen when a future spacecraft (Cassini?) completes this photography.
Perhaps the most basic explosion indicator is that all fragments of significant mass will trap smaller nearby debris from the explosion into satellite orbits. So explosions tend to form asteroids and comets with multiple nuclei of all sizes. Collisions, by contrast, normally cannot produce fragments in orbits because any debris orbits must lead either to escape or to re-collision with the surface.
Over 100 additional lines of evidence related to the eph and the standard models it would replace are summarized in [iii].
Did More Than One Planet Explode?
Many lines of evidence suggest more than one planetary explosion in the solar system’s history.
The discovery of one, and probably two, new asteroid belts orbiting the Sun beyond Neptune is especially suggestive, given that the main asteroid belt is apparently of exploded planet origin. Evidence of the “late heavy bombardment” in the early solar system is another strong indicator. These points are discussed later in this article.
On Earth, geological boundaries are accompanied by mass extinctions at five epochs over the last billion years. Two of the most intense of these, the P/T boundary about 250 Mya, and the K/T boundary (and the extinction of dinosaurs) at 65 Mya, are the most likely to be associated with the damage to Earth’s biosphere expected from a major planet explosion.
Meteorites provide direct evidence about their parent bodies. Yet this evidence strongly indicates at least 3-4 distinct parent bodies. Oxygen isotope ratios are generally similar for related planetary bodies, such as all native Earth and Moon rocks. These ratios for meteorites require at least two distinct, unrelated parent bodies, and probably more.
The data show clusterings of exposure ages around several different primary epochs, suggesting multiple explosion epochs.
Main belt asteroids come in many types, but most of these are sub-type distinctions. 80% of all main belt asteroids are of type C (“carbonaceous”), and most of the remaining 20% are of type S (“silicaceous”). The former are found predominately in the middle and outer belt, while the latter are mostly in the inner belt, the part that lies closest to Mars. These two types are unlikely to have had the same parent body.
Finally, it should be noted that we can estimate the total mass of the body that exploded to produce all the comets seen today. (The lifetime of those comets is limited to 10 million years by galactic tidal forces and planetary perturbations.)
Explosion Signatures in the Main Asteroid BeltIn Figure 2, we show a plot of average orbital eccentricity (called “proper eccentricity”) versus average mean distance (called “proper semi-major axis”) for thousands of main-belt asteroids.
However, as these same comets recede again far from the planets, the clustering property is virtually destroyed, as shown on the right side of Figure 3. The scattering is so great that no clustering near –5 or any other value will exist the next time around. So these comets must have been making their first visit to the planetary part of the solar system. For that reason, they are called “new comets”.
These new comets, first noted by Oort, were notthe belt of comets beyond Pluto expected by the primeval solar nebula hypothesis. They arrive from all directions on the sky, with no tendency to be concentrated toward the plane of the planets. Also, they move in directions opposite to the planets as often as in directions consistent with the planets.
In the standard model with an Oort cloud of comets, there is no obvious way to tell the difference between comets anywhere in the energy parameter range on the left side of Figure 3. So there is no reason for any observational class of comet to be other than randomly distributed among all the comets in that figure. If all the orbits could be improved to class 1A, the overall average appearance of the distribution ought to be unchanged.
However, in the eph, the real distribution would have all the comets in a single bin, and all the observed spread of energy parameter values would be due to observational error.
And if all the comets of classes 1B, 2A and 2B were improved to class 1A, the whole distribution should narrow greatly. Opik’s test was to separate comets of class 1A from the other classes to determine if the distribution was significantly broader for the other classes than for class 1A (indicating theeph is right), or essentially the same for both groups (indicating the Oort cloud is right).
The results are shown on the left side of Figure 4 for new class 1A comets and on the right side of the same figure for new comets of classes 1B, 2A and 2B.
The left side shows 2.6 times as many comets in the central spike as in the immediately adjoining bins combined. The right side shows only 0.8 times as many comets in the central spike as in the two adjoining bins, and has a clearly broader distribution.
The Opik test is cleanly passed by the exploded planet hypothesis (eph), but not by the Oort cloud model.
Comets (at least most of them) acquired their extremely elongated, planet-crossing orbits by ejection in an explosion that we can now date at 3.2 million years ago. New comets are the continuing rainback of debris from that explosion.
Satellites of Asteroids and Comets
If asteroids and comets are the products of accretion from a nebula, or even from collisional break-ups, they will invariably be isolated single bodies because their gravitational fields are too weak to effect captures.
For example, in a break-up event, most debris escapes, and what does not falls back onto the surface it was ejected from after one orbit. Even if it managed to barely miss the surface, tidal forces would bring it back down in short order.
By contrast, in the eph, space is filled with debris just after the explosion. Large fragments will find lots of debris inside their gravitational spheres of influence, and these will remain in stable orbits as permanent satellites of these larger fragments. For that reason, I presented papers at the International Astronomical Union meeting in Argentina in 1991, and the Flagstaff meeting of asteroid, comet, and meteorite experts in that same year, pointing out the eph prediction.
Specifically, spacecraft visiting asteroids (or comets) should find at least one of the larger debris bodies (satellites) in orbit around the asteroid (or comet) primary nucleus. This prediction, also published in [iii] and [iv], was considered extremely unlikely by mainstream astronomers, one of whom made a public wager with me that it would not happen.
The Galileo spacecraft flew by asteroid Ida in 1993, and returned images showing a 1-km satellite (now named Dactyl) in a stable orbit around its nucleus. Since that discovery, two telescopic discoveries of satellites of other asteroids have been made. [v] This supplements occultation and radar evidence of long standing suggesting asteroid satellites.
The two blocks are areas where contrast was stretched for better visibility of the “roll mark”. The image appears to show a track starting in a random location, going up the outside wall of a crater, down the inside wall, and ending in a 50-meter boulder. Many additional examples of boulders, tracks, and boulders at the ends of tracks can be seen in later spacecraft images.
In the meantime, evidence for comet satellites was mounting as well. The Giotto spacecraft was the first to approach a comet, where it found “brightness concentrations” in the inner coma referred to as “dust spikes”. [vii] Then Hubble Space Telescope observations of Comet Hale-Bopp showed at least one, and probably three secondary nuclei orbiting the primary comet nucleus. [ii]
Another strong test distinguishing the eph from the standard models comes from comet split-velocity data.
It ought to be easy to distinguish these two extreme possibilities from observations. And indeed, it is. One of the strongest such tests follows.
Some comets are observed to “split” into two or more comets. That was unexpected behavior in the dirty snowball model, but is explained after the fact as the breaking apart of the snowy nucleus under the action of strong jets.
“Splitting” is required by the satellite model because, as the comet approaches the Sun and its gravitational sphere of influence shrinks, some outer satellites may find themselves outside the sphere of influence. Such objects then escape into independent solar orbits. The escape event will appear to a distant observer as a “split” of the comet into two or more pieces.
The test involves the velocity of the fragment comets relative to the original comet from which they split. In the dirty snowball model, the velocity is the result of jet action. The energy source might be entirely internal to the comet, in which case the velocity of ejection of split comet fragments will be independent of the distance from the Sun at which the split occurs.
The laws of dynamics require that “split” fragment velocities be escape velocities, which vary inversely with the square root of solar distance. Any other observed relationship would falsify the model.
In Figure 6, we show a plot of split-comet component relative velocities, V, versus solar distance of the comet in astronomical units at the time of splitting, R, on a log-log scale. The data and its one-sigma spread lie within the shaded region. For comparison, three theoretical curves are shown, labeled “C”, “S”, and “E”.
These represent a comet-internal energy source, a solar energy source, and gravitational escape energies as predicted by the eph, respectively. All curves have been shifted vertically to intersect at 1 au (about 150 million kilometers) because only the slopes are relevant.
It is apparent that the theoretical curve predicted by the eph model falls within the one-sigma data region, and is therefore fully in accord with the observations. Both of the possibilities for the dirty snowball model fall well outside the data range by at least four sigma. This means the dirty snowball model is excluded as an explanation at the statistical level of better than 10,000-to-1.
In summary, we see that the satellite model for the nature of comets, based on the eph model for the origin of comets, is consistent with the observational data; whereas the standard model is strongly excluded by the data.
Planetary and moon explosions are not just a recent phenomenon.
“[The late heavy bombardment] occurs relatively late in the accretionary history of the terrestrial planets, at a time when the vast majority of that zone’s planetesimals are already expected to have either impacted on the protoplanets, or been dynamically ejected from the inner planets region.”
“It appears that a flux of impactors flooded the terrestrial planets region at this point in the solar system’s history, and is preserved in the cratering record of the heavily cratered terrain on each planet.”
“An essential requirement of any explanation for the late heavy bombardment is that the impactors be ‘stored’ somewhere in the solar system until they are suddenly unleashed about 4.0 Gyr ago.”
“A plausible explanation for the late heavy bombardment remains something of a mystery.”
“…it seems likely that the late heavy bombardment is not the tail-off of planetary accretion but rather is a late pulse superimposed on the tail-off. Nor is there any reason to suppose that it was the only such pulse; it may have been preceded by several others which are not easily discernible from it in the cratering record.”
The following documented geological events at the terrestrial K/T boundary at 65 Mya can easily be associated with a planetary explosion event, most likely the explosion of “Planet V” near the present-day orbit of Mars.
- two boundary layers (ash and clay) of global extent
- at least eight known major impact craters across globe from that epoch
- “hot zones” of radioactivity found in Africa at the K/T boundary
- the Deccan Traps in India – the 2nd largest episode of volcanism in Earth history
- changes in atmospheric and ocean composition
- a single global fire
- the extinction of 70% of all terrestrial species
- the absence of corresponding layers in the Antarctic
Evidence that Mars is a former moon:
- Mars is much less massive than any planet not itself suspected of being a former moon
- Orbit of Mars is more elliptical than for any larger-mass planet
- Spin is slower than larger planets, except where a massive moon has intervened
- Large offset of center of figure from center of mass
- Shape not in equilibrium with spin
- Southern hemisphere is saturated with craters, the northern has sparse cratering
- The “crustal dichotomy” boundary is nearly a great circle
- North hemisphere has a smooth, 1-km-thick crust; south crust is over 20-km thick
- Crustal thickness in south decreases gradually toward hemisphere edges
- Lobate scarps occur near hemisphere divide, compressed perpendicular to boundary
- Huge volcanoes arose where uplift pressure from mass redistribution is maximal
- A sudden geographic pole shift of order 90° occurred
- Much of the original atmosphere has been lost
- A sudden, massive flood with no obvious source occurred
- Xe129, a fission product of massive explosions, has an excess abundance on Mars
Putting all this evidence together, we have strong hints for two original planets near what is now the main asteroid belt: hypothetical “Planet V” and “Planet K”.
We have hints of two more asteroid belts, probably from the explosions of two more planets (“Planet T” and “Planet X”) beyond Neptune. And we have hints for two extra-large gas giant planets, “Planet A” and “Planet B”, that exploded back near the solar system beginning.
Of the existing nine major planets today, we have strong evidence that Mercury is an escaped moon of Venus[xi], Mars is an escaped moon of Planet V, and Pluto and its moon Charon are escaped moons of Neptune[xii]. If we eliminate these, then perhaps the original solar system consisted of 12 planets arranged in 6 “twin” pairs. Such an arrangement would be consistent with origin of all major planets and moons by the fission process. [xiii]
The most frequently asked question about the eph is “What would cause a planet to explode?”
- The earliest and simplest theoretical mechanism is that of Ramsey[xiv], who noted that planets must evolve through a wide range of pressures and temperatures. This is true whether they are born cold and heat up under gravitational accretion, or born hot and cool down by radiation of heat into space.During the course of this evolution, temperatures and pressures in the cores must occasionally reach a critical point, at which a phase change (like water to ice) occurs. This will be accompanied by a volume discontinuity, which must then cause an Earth-sized or smaller planet to implode or explode, depending on whether the volume decreases or increases.
- The second explosion mechanism, natural fission reactors, is currently generating some excitement in the field of geology. [xv] Auranium mine at Oklo in the Republic of Gabon is deficient in U-235 and is accompanied by fission-produced isotopes of Nd and Sm, apparently caused by self-sustaining nuclear chain reactions about 1.8 Gyr ago. Later, other natural fission chain reactors were discovered in the region. Today, uranium ore does not have this capability because the proportion of U-235 in natural uranium is too low.But 1.8 Gyr ago, the proportion was more than four times greater, allowing the self-sustaining neutron chain reactions. Additionally, these areas also functioned as fast neutron breeder reactors, producing additional fissile material in the form of plutonium and other trans-uranic elements. Breeding fissile material results in possible reactor operation continuing long after the U-235 proportion in natural uranium would have become too low to sustain neutron chain reactions.This proves the existence of an energy source in nature able to produce more than an order of magnitude more energy than radioactive decay alone. Excess planetary heat radiation is said to be gravitational in origin because all other proposed energy sources (e.g., radioactivity, accretion, and thermonuclear fusion) fall short by at least two orders of magnitude. But these natural reactors may be able to supply the needed energy. Indeed, nuclear fission chain reactions may provide the ignition temperature to set off thermonuclear reactions in stars (analogous to ignition of thermonuclear bombs).
- The third planetary explosion mechanism relies on one other hypothesis not yet widely accepted, but holds out the potential for an indefinitely large reservoir of energy for exploding even massive planets and stars. If gravitational fields are continually regenerated, as in LeSage particle models of gravity [xvi], then all masses are continually absorbing energy from this universal flux.Normally, bodies would reach a thermodynamic equilibrium, whereat they radiate as much heat away as they continually absorb from the graviton flux. But something could block this heat flow and disrupt the equilibrium. For example, changes of state in a planet’s core might set up an insulating layer. In that case, heat would continue to be accumulated from graviton impacts, but could not freely radiate away. This is obviously an unstable situation. The energy excess in the interior of such a planet would build indefinitely until either the insulating layer was breached or the planet blew itself apart.
We have covered most of the successful predictions of the exploded planet hypothesis mentioned in the abstract:
(1) satellites of asteroids(2) satellites of comets(4) “roll marks” leading to boulders on asteroids(6) explosion signatures for asteroids(7) strongly spiked energy parameter for new comets(8) distribution of black material on slowly rotating airless bodies(9) splitting velocities of comets(10) Mars is a former moon of an exploded planet
”The existence of a water-soluble salt in this meteorite is astonishing,” wrote R.N. Clayton of the University of Chicago in the reference cited.
True, unless one had the exploded planet hypothesis in mind.
Supplementing the idea of salt water in meteorites, we did explicitly predict salt water in comets. [xviii]
“In March, a long sodium tail was discovered in Comet Hale-Bopp. Aside from the general interest in this new type of comet tail, it was noted that the sodium ions have a half-life of just half a day, too short to survive a trip from the nucleus to the farthest parts of the tail.So the sodium must be conveyed as part of a parent molecule that is split by the solar wind into sodium and some other ions. The significance of this for comet models is that the exploded planet hypothesis says that comets originated in the explosion of a water-bearing planet. If that planetary water was salt water, as planetary oceans on Earth all tend to be, then water in comets would be salt water.The parent molecule for the salt escaping the comet’s coma into the tail would be sodium chloride (salt), and the “other ions” would be chlorine ions. The unknown parent molecule has not yet been officially discovered. But one can readily see that the discovery of chlorine in comets to go along with this discovery of sodium would make a strong case for the planetary origin scenario.”
With the documented track record the eph has now established, it is small wonder that professional astronomers are no longer willing to make wagers with eph proponents about the outcome of either recent or future eph predictions.
[i] T. Van Flandern (1978), “A former asteroidal planet as the origin of comets”, Icarus 36, 51-74.
[ii] Z. Sekanina (1999), “Detection of a satellite orbiting the nucleus of Comet Hale-Bopp (C/1995 O1)”, Earth, Moon & Planets in press.
[iii] T. Van Flandern (1993; 2nd edition 1999), Dark Matter, Missing Planets and New Comets, North Atlantic Books, Berkeley, 215-236; 178.
[iv] T. Van Flandern (1992), “Minor satellites and the Gaspra encounter”, Asteroids, Comets, Meteors 1991, LPI, Houston, 609-612.
[v] 3671 Dionysus (1997), Sci.News 152, 200; 45 Eugenia (1999), Science 284, 1099-1101.
[vi] T. Van Flandern (1999), “Status of ‘the NEAR challenge’”, MetaRes.Bull. 8, 31-32. Also at <http://metaresearch.org>.
[vii] T. LeDuin, A.C. Levasseur-Rigourd & J.B. Renard (1993), “Dust and gas brightness profiles in the Grigg-Skjellerup coma from OPE/Giotto”, in Abstracts for IAU Symposium 160: Asteroids, Comets, Meteors 1993, Belgirate (Navara) Italy, 182.
[viii] E. Marchis, H. Bochnhardt, O.R. Hainaut & D. Le Mignant (1999), “Adaptive optics observations of the innermost coma of C/1995 O1: Are there a ‘Hale’ and a ‘Bopp’ in comet Hale-Bopp?”, Astron.Astrophys. 349, 985-995.
[ix] P.R. Weissman (1989), “The impact history of the solar system: implications for the origin of atmospheres,” in Origin and Evolution of Planetary and Satellite Atmospheres, S.K. Atreya, J.B. Pollack, and M.S. Matthews, eds., Univ. of Arizona Press, Tucson, 247-249.
[x] E.H. Christiansen & W.K. Hamblin (1995), Exploring the Planets, 2nd ed., Prentice Hall, Englewood Cliffs, NJ, 144.
[xi] T.C. Van Flandern & R.S. Harrington (1976), “A dynamical investigation of the conjecture that Mercury is an escaped satellite of Venus”, Icarus 28, 435-440.
[xii] R.S. Harrington & T.C. Van Flandern (1979), “The satellites of Neptune and the origin of Pluto”, Icarus 39, 131-136.
[xiii] T. Van Flandern (1997), “The original solar system”, MetaRes.Bull. 6, 17-29. See also <http://metaresearch.org>.
[xiv] W.H. Ramsey (1950), “On the instability of small planetary cores (I)”, Mon.Not.Roy.Astr.Soc. 110, 325-338.
[xv] (1998), EOS 79 (9/22), 451 & 456. See also <http://www.ans.org/pi/np/oklo/>.
[xvi] T. Van Flandern (1996), “Possible new properties of gravity”, Astrophys.&SpaceSci. 244, 249-261.
[xvii] (1999), Science 285, 1364-1365 & 1377-1379:
[xviii] T. Van Flandern (1997), “Comet Hale-Bopp update”, MetaRes.Bull. 6, 29-32: [The author gratefully acknowledges Richard Hoagland of the Enterprise Mission for this argument.]
[xix] E. Lyytinen (1999), “Leonid predictions for the years 1999-2007 with the satellite model of comets”, MetaRes.Bull. 8, 33-40; T. Van Flandern (1999), “1999 Leonid meteor storm – How the predictions fared”, MetaRes.Bull. 8, 59-63.
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