"Rapid burial beneath many kilometers of sediment produces instantaneous pressure increases, but once again it takes too much time to heat the sediment. In fact it would take many millions of years to heat up sediment buried 20 kilometers beneath the surface." — Kurt Wise, First International Conference on Creationism, 19861
"Convective flows of hydrothermal fluids might be capable of moving and dissipating heat from granitic plutons, but an additional, as yet unknown mechanism would have been needed to remove the heat generated by the accelerated radioisotope decay." — Andrew Snelling, RATE Volume II, 20052
Summary
The five articles in this group ask one question about five kinds of rock: can the igneous and metamorphic rocks that young-earth models place in the Flood year form, cool and, where they now stand at the surface, be uncovered inside that year? This overview puts their answers side by side. It adds no new research except where two of the articles disagree, and Part 9 settles those two points from the sources.
The young-earth models give three mechanisms, and Part 1 quotes each in its authors' words. Catastrophic plate tectonics supplies the setting and the speed. Hydrothermal convection, water circulating through hot rock, is the proposed way to cool a batholith fast; its one published model gives "a mere 3,000 years."3 Accelerated nuclear decay is the clock behind the shortest figure, granite "solidified and cooled in just 6 to 10 days,"4 and its own author concedes that it adds heat that "an additional, as yet unknown mechanism" would have to remove.2
The overall verdict. The young-earth side is right about the parts that can be watched or reproduced. Magma rises fast, single lava flows are built in years, and metamorphic reactions run in days in the laboratory. It is also right that the global heat of these rocks is small next to the ocean-floor heat its own physicists already face. It fails on moving heat through thick rock. Each of the four articles that prices a time finds a Flood year short, by a factor of about thirty for Devils Tower at the friendliest arithmetic and by up to ten million for batholiths and metamorphic belts.
One line per article.
- Granite Cooling: the one young-earth thermal model gives 3,000 years to shed three quarters of the heat and declines to claim a Flood year. Conduction takes 10⁵ to 10⁷ years for a body kilometres thick, a one-year batholith would need 28 to 70 darcies of permeability, and the zircon and helium clocks in the rock record tens of millions of years of cooling.
- Metamorphic Rocks: the reactions are fast, as Kurt Wise said in 1986, and heating 20 km of rock is not. Conduction takes 1.3 to 12.7 million years, hot water would need a crust a million times more permeable than the one measured, and the one young-earth number, 12 to 20 days for Cooma, contains no heat calculation.
- Flood Basalts: single flows are fast and the heat of the Columbia River basalts is six millionths of the ocean-floor heat. Between the flows lie root-traced soils, an 840-year varved lake, Deccan lakes and turtle eggshells, and the creationist literature is split on whether these basalts erupted in the Flood at all.
- Devils Tower and Volcanic Landforms: the Tower's 2 to 3 m columns record slow cooling. The fastest published mechanism gives 16 to 45 years and conduction 1,000 to 5,000. No exposure age has been measured by either side, and at measured outcrop erosion rates the Tower survives 5 to 10 million years.
- Polonium Radiohalos: the halos are real and uranium-free, but the polonium was delivered by fluids, not created. RATE's version of that model needs accelerated decay, and a halo records how many decays occurred, not how long they took.
Two findings appear only when the articles are read together.
- Every fast route runs through water, and water waits for cracks. In Anthony Lamur and colleagues' experiments the joints in cooling lava open at 840 to 890 °C, "regardless of the imposed cooling rate."5 The water that quenches a basalt flow follows "just behind the lava solidification front."6 Lister's estimate for the cracking front in a cooling intrusion is about 30 m a year.7 At 15 km the crust is 2,800 times too tight to carry the water that would heat a metamorphic belt in a year, even at the highest transient permeability ever inferred.8 Part 8 sets the numbers side by side.
- Every Flood-year figure in the young-earth literature for these rocks traces back to the polonium halos or to a misreading of the one thermal model. The 6 to 10 days for granite comes from polonium half-lives, not from a heat calculation.2 The 12 to 20 days for Cooma is two of those added together.9 The "couple of months" in Walker 2003 cites a paper whose answer is 3,000 years.10 Devils Tower and the flood basalts have no young-earth cooling time at all. So the case for cooling inside the Flood year rests on one argument, and the polonium article finds that a halo measures dose, not time.
Verdict. The events are fast and the global heat is affordable. The cooling is not fast. Conduction, convection, column widths, soils between flows and the clocks inside the rocks all put these bodies at decades to tens of millions of years, and no young-earth thermal calculation for any of the five reaches a Flood year.
Part 1: The young-earth models, in their own words
Each position below is quoted from its primary source, through the child article that read and verified it, before anything is priced.
The movement's own statement of the problem
Kurt Wise put the problem to the first International Conference on Creationism in 1986, and he split it in two. The reactions are fast: "Chemical equilibrium in the process of metamorphism is thus rather quickly reached once the thermal conditions are achieved. It is, however, rather difficult to achieve those conditions."1 The heat is slow: "it would take many millions of years to heat up sediment buried 20 kilometers beneath the surface."1 Andrew Snelling's founding paper on metamorphism agreed eight years later: "the biggest problem creationists face with the conventional scenario for regional metamorphism is the heat presumed to have been involved".11 Most of the young-earth papers quoted below try to answer it.
Catastrophic plate tectonics: the setting
The 1994 paper that launched catastrophic plate tectonics, by Steven Austin, John Baumgardner, Russell Humphreys, Andrew Snelling, Larry Vardiman and Kurt Wise, does not model these rocks. It says that Flood models "claim that it is possible on a short timescale to explain the cooling of plutons and ocean plate material; regional metamorphism (see, for example, Snelling)",12 and leaves the work to Snelling. Snelling's own model leans on the same setting: "only moderate temperatures may be needed," generated "due to the thicknesses of the sediment piles catastrophically accumulated, and due to the increased heat flow from the mantle because of rapid plate tectonics."11 Baumgardner later offered the high-pressure blueschists of California as support, because their return to the surface is a "difficulty" that "disappears in the CPT framework because the subduction and exhumation velocities are orders of magnitude higher".13 Michael Oard adds that fast plates could create "greater tectonic pressure at shallow depths," so a rock that records high pressure need not have been deep.14
Catastrophic plate tectonics also sets the scale of the heat. William Worraker, a young-earth physicist, totals the heat of every large igneous province at "not exceeding 4.0 × 10²⁶ J" and calls it "insignificant in comparison with the heat deposition involved in forming the ocean floors (1.4 × 10²⁹ J)", then adds that the local impact "would have been highly dramatic in the absence of some special, hitherto unrecognized, cooling mechanism."15 The ocean-floor heat itself is the subject of The Heat Problem and Catastrophic Plate Tectonics, and this group does not re-argue it.
Convective cooling: the route
The one young-earth thermal model of a batholith is Snelling and John Woodmorappe's of 1998. Conduction alone "needs a few million years to cool" a body 16.5 km thick, "But with the intensity of convective cooling that is allowed by a permeability K of 10 millidarcies (easily exceeded—see below), the time to cool this batholith falls to a mere 3,000 years."3 The paper is careful about what that number means. It ends "at 25% of the difference between ambient temperatures and solidus temperature."3 It concedes that "the permeability of a granite in the actual process of cooling remains unknown."3 It lists its own unfinished work: the rates at which Flood tectonism cracks the rock open and the rock heals "need to be quantified."3 And it declines to claim a Flood year: "This discussion does not imply that all of the large batholiths had cooled by the time they were uplifted after the Flood."3
Water is the cooling route in the other children too. Tim Clarey writes of Devils Tower that "During the Flood, groundwater percolating along the open fractures likely caused the lower part of the magma to cool quickly."16 Of the Columbia River basalts he writes that tsunamis were "crashing across Oregon and Washington and over the tops of the fresh lava flows, quenching the molten centers and forming entablature."17
Accelerated decay: the clock
The shortest numbers come from the RATE project, and they come from radiohalos. Snelling and Mark Armitage's 2003 count found uranium halos beside polonium halos in the same granites, and concluded that "at least 100 million years worth (at today's rates) of accelerated radioactive decay has occurred."18 Snelling's popular summary: "In other words, the radioactive decay of uranium was formerly up to a billion times faster than it is today!" and "polonium halos mean that the granites solidified and cooled in just 6 to 10 days!"4 He is explicit about where the figure comes from: "this timescale is constrained by the half-lives of these isotopes, and not by the assumption that these granites formed during the Flood year."2 His one number for a metamorphic terrane builds on it: the Cooma complex in New South Wales "only required 12–20 days, based on the catastrophic granite formation of the adjacent Murrumbidgee Batholith".9
The same authors state the cost. In 2005: "an additional, as yet unknown mechanism would have been needed to remove the heat generated by the accelerated radioisotope decay."2 In 2023: "One major objection raised is the huge amount of heat (as well as radiation) that would seem to be generated by the pulse of accelerated ²³⁸U decay."19
Where the models put each rock body
The models do not place all five in the same part of the Flood, and for one of them they do not agree with each other.
- Granite batholiths are Flood intrusions in Snelling's papers. They cool in days in his later papers and over as much as 3,000 years in the 1998 one. Robert Gentry, who started the polonium argument, treated the Precambrian granites holding his halos as created rocks; Snelling rejects that on field evidence.9
- Regional metamorphic belts such as Cooma are Flood products in Snelling's papers, made by the heat and water of Flood granites.
- Flood basalts are placed three ways. Austin reads the trend in eruption size as "the declining power with time of post-Flood volcanoes."20 John Morris puts them "probably occurring during the very last stages of the Flood or in the years of readjustment to follow".21 Woodmorappe, Oard and Clarey put them inside the Flood: "The Columbia Plateau lavas erupted near the end of the Flood's receding phase (Miocene)."17
- Devils Tower is a receding-phase intrusion for Clarey: "these magmas formed during the receding phase of the Flood after most of the sediments were deposited."16 Its exposure is "4,500 years ago during the draining of the floodwaters."16 Oard argues that it "should have been destroyed quickly, surely in less than 100,000 years."22
- Polonium halos sit in the granites of item 1, and RATE uses them as the clock for item 1 and, through Cooma, for item 2.
Only bodies placed inside the Flood owe an answer to a one-year budget. For Devils Tower the budget is tighter still: the body had to cool and joint before the receding water stripped its cover, so the budget is months.
Part 2: Granite cooling
Granite Cooling grants the young-earth side three things, all about emplacement. Granite magma can rise in a way that is "geologically extremely rapid—perhaps even catastrophic,"23 plutons are built from many sheets, and water cools rock faster than conduction does. It then finds that Snelling and Woodmorappe's 3,000 years is Cathles' chart correctly rescaled, that it measures the time to shed three quarters of the temperature contrast, and that it is 3,000 Flood years. Conduction by Jaeger's 1957 coefficient, 0.016 D² years for a sheet D metres thick, gives 400,000 years for 5 km and 6.4 million for 20 km,24 under a ceiling of 4 million years for any intrusion within 5 km of the surface.7 A batholith that reached the 75 per cent mark in a year would need 28 to 70 darcies through its whole thickness, against 1 to 100 millidarcies measured in granite and about 10 darcies as Lister's theoretical maximum. The rock's own clocks agree: zircon ages across the Tuolumne suite in Yosemite span "at least 10 m.y.,"25 and five clocks in one Alaskan sample read in closure-temperature order, "a remarkably smooth hyperbolic cooling history for this sample since crystallization at 60 Ma".26 The article's verdict is that a Flood year misses by three to seven orders of magnitude.
Part 3: Metamorphic rocks
Metamorphic Rocks grants that the reactions are fast, that the mainstream's simple conductive model fails for short mountain-building events, and that tectonic overpressure is real. None of these touches the temperature. Heat crosses 20 km of rock by conduction in 1.3 to 12.7 million years and gets about 11 metres into rock in a year.27 Hot water would need about 1.5 darcies through 15 km of crust, where the measured mean permeability is nine hundred thousand times lower.8 The fast mainstream results the young-earth side cites sit inside slow histories: in Barrow's own zones in Scotland "the thermal peak conditions lasted for only 200–300 kyr" inside a "10–15 Ma orogeny,"28 and the field defines short-duration regional metamorphism as under ten million years.29 Snelling's 12 to 20 days for Cooma adds two granite timescales and computes no heat transfer, and the paper he cites for Cooma's cooling found it "more consistent with the unroofing of a regional thermal high than cooling of an igneous intrusion."30
Part 4: Flood basalts
Flood Basalts finds the young-earth side right on three points. Single flows are fast: the Roza Member's 1,300 km³ "was constructed over a period of at least 14 years."31 Water touched the flows, and the global heat is small. The problem is the time between flows. The red layers between Columbia River flows are "paleosols that record significant hiatuses in basalt flow emplacement,"32 one lake dammed by a flow holds "~840 yr of deposition,"33 and Deccan lakes and turtle eggshells sit between flows there. At the sustained rates measured for the Roza Member and the Deccan groups, the Columbia River pile alone takes over 2,000 years of continuous eruption, where a Flood year needs 575 km³ a day. The fastest burst rate, over 1,000 km³ a year, cuts the eruption to 210 years but comes with hiatuses of centuries to millennia between bursts. Each 30 m flow takes 4.2 to 17 years to solidify. The article finds that the within-Flood placement of Woodmorappe, Oard and Clarey fails, and that Austin's post-Flood placement survives the year only by giving up the basalts as Flood evidence.
Part 5: Devils Tower and volcanic landforms
Devils Tower and Volcanic Landforms finds no young-earth cooling time to test, because the young-earth argument about the Tower is about its exposure. Column width is a cooling-rate gauge: "the column radius and stria size are proportional to each other and inversely proportional to the cooling rate of the lava."34 The Tower's 2 to 3 m columns,35 priced by Goehring and Morris's relation with water in the cracks, give a jointing front of about 2.8 to 5.5 m a year and 16 to 45 years for the body. A one-year crossing would need columns about 8 cm across. Conduction gives 1,000 to 5,000 years for the shapes anyone proposes, and the three-dimensional model of the authors who argue the Tower was never deeply buried gives "∼4000 yr."35 On exposure Oard is right that no exposure age has been measured, but at the measured median outcrop erosion rate of 5.4 m per million years36 the Tower loses 27 to 54 m of a 114 to 152 m radius in 5 to 10 million years and survives. A beryllium-10 exposure age would settle it, and nobody has measured one.
Part 6: Polonium radiohalos
Polonium Radiohalos finds the halos real: an independent laboratory confirmed in 1976 that "no or only small amounts of uranium are present in polonium halos."37 It then finds that the polonium was delivered by fluids. Gentry's own 1976 paper,38 the vein dikes and uranium-mine pegmatite at his Ontario sites,39 and RATE's own count of two polonium-218 halos against 1,857 polonium-21018 all point that way, and Snelling and Armitage wrote that Gentry's primordial hypothesis "has been falsified".18 For this group the decisive finding is that a halo records dose, not time. On that article's own estimate, one 10 µm zircon at 1,000 parts per million uranium supplies a billion polonium atoms in about 500 million years at today's rates, or in days at ten billion times that rate, and the halo cannot tell which. The 6 to 10 days also rests on an annealing ceiling read only in abstract, where halos fade at 134 °C and are gone at 151 °C,40 and on a transport model whose author predicted in 2000 that it should give "67,000 ²¹⁰Po radiohalos for each ²¹⁸Po radiohalo" and has never addressed the gap since.41
Part 7: The five rock bodies side by side
Every number below is carried over from the child article named in the first column. Figures marked † are that article's own arithmetic, with every input printed there.27
| Rock body | The young-earth claim | The physical constraint | What the article concluded | What would change the verdict |
|---|---|---|---|---|
| Granite batholith. Snelling and Woodmorappe's 16.5 km body; the Sierra Nevada | A Flood intrusion. 3,000 years to the 75 per cent mark at 10 millidarcies (1998). 6 to 10 days, from radiohalos (2005, 2008). | Heat: 1.7 × 10²⁴ J for the California arc, 105 W/m² over the whole Earth for a year.† Rate: 28 to 70 darcies through the whole body,† against 1 to 100 millidarcies measured and 10 darcies as Lister's theoretical maximum. Lister's cracking front, 30 m a year, needs 275 years to reach the centre. | Conduction 10⁵ to 10⁷ years; convection at any permeability measured or proposed 10⁴ to 10⁵; zircon and helium clocks record tens of millions of years. A Flood year is three to seven orders of magnitude short. | A published mechanism that keeps tens of darcies open through still-ductile rock for a year and disposes of the steam. An accelerated-decay model that predicts the closure-temperature order of the clocks. |
| Regional metamorphic belt. Barrow's zones in Scotland; Cooma, New South Wales | A Flood product. "Moderate temperatures" from thick sediment and rapid plate tectonics (1994). 12 to 20 days for Cooma (2008). | Heat, for scale only: 1.2 × 10²² J for the Barrovian type area, 2.1 × 10⁵ W/m² over 1,800 km² for a year; 6.4 × 10⁶ W/m² for Cooma on Snelling's own 300 km² and 16 days.† Rate: conduction reaches 11 m in a year; water needs about 1.5 darcies through 15 km, 2,800 times the highest transient permeability inferred; friction needs about 68 km of slip.† | Each route misses a Flood year by 10³ to 10⁷. The mainstream's fastest durations, 10⁵ to 10⁷ years, sit inside longer histories. Cooma's 12 to 20 days contains no heat calculation. | One traverse across a Barrovian isograd with an independent thermometer, testing Snelling's "moderate temperatures." A model showing catastrophic plate tectonics opening crust-scale permeability. |
| Flood-basalt pile. The Columbia River and Deccan provinces | Placed three ways: the Flood's receding phase (Woodmorappe, Oard, Clarey), its last stages or the years after (Morris), or after it (Austin). | Heat: 8.7 × 10²³ J for the Columbia River basalts, 6 × 10⁻⁶ of the ocean-floor heat, but 131,000 W/m² over the plateau for a year.† Rate: 575 km³ of lava a day for a year, against Laki's 12.3 km³ in eight months; a 30 m flow solidifies in 4.2 to 17 years.† | Single flows are fast and the global heat is small. Soils with roots, an 840-year lake, Deccan lakes and eggshells between flows need centuries to tens of thousands of years per province. The within-Flood placement fails; the post-Flood placement survives the year but stops treating the basalts as Flood deposits. | Showing that the interflow soils are not soils and the Clarkia laminae not annual, against their roots, peat, snails and leaf-bearing layers. A young-earth cooling time for water-quenched flows. Reidel's whole-province count of interbeds would sharpen the arithmetic either way. |
| Devils Tower. A 250 m phonolite body at 850 °C | A receding-phase intrusion, exposed "4,500 years ago during the draining of the floodwaters." No cooling time published. | The body had to joint before its cover was stripped, so the budget is months. Rate: the jointing front read from 2 to 3 m columns moves 2.8 to 5.5 m a year; crossing in one year needs columns about 8 cm wide.† Exposure: outcrops erode at a median 5.4 m per million years. | 16 to 45 years by the fastest mechanism, 1,000 to 5,000 by conduction,† about 4,000 in Závada's model. A factor of thirty short at the friendliest arithmetic and thousands at the standard one. Exposure is open, and the arithmetic favours the long exposure. | A beryllium-10 exposure age on the summit and the largest talus blocks. A mechanism that grows wide columns fast, against the width-to-rate relation. |
| Polonium halos in granite biotite | Gentry: primordial polonium in created granite. RATE: polonium carried by hot fluid during accelerated decay, with the granite below about 150 °C within 6 to 10 days. | Dose: 500 million to a billion alpha decays per halo. Supply: one 10 µm zircon at 1,000 ppm uranium makes a billion polonium atoms in about 500 million years at today's rates.† Annealing: halos fade from 134 °C and are gone at 151 °C. | The halos are real and uranium-free. The polonium was delivered, not created, and the RATE count says so. A halo records dose, not time, so it cannot time the cooling. | Brawley's photometric test showing that three-ring halos are not radon halos. Feather's 1978 biotites, where polonium-218 halos are said to outnumber polonium-210. The full Laney and Laughlin table. |
The table's third column carries the one point all five share. Total heat is the lesser constraint wherever it is set against the whole Earth. What binds is rate: how fast heat can be conducted, how fast rock cracks to let water in, how much power one region must shed, how fast lava can erupt, how fast soils and lakes form between flows, and how fast a halo's dose accumulates from its supply.
Part 8: Where the numbers meet
Water waits for the crack
Every young-earth route to fast cooling is water. Snelling and Woodmorappe's convection, Clarey's groundwater at Devils Tower and his tsunamis on the Columbia Plateau all depend on it. Four children, working on four kinds of rock, found the same limit on it: water reaches hot rock only through cracks and pores, and in hot rock these open slowly or not at all.
- In lava, Lamur and colleagues found that the joints open at 890 to 840 °C "regardless of the imposed cooling rate."5 Devils Tower reads the speed of the jointing front from the width of the columns it leaves.
- In a basalt flow, Long and Wood's water-quench model works only "provided that the infiltration front moves downward just behind the lava solidification front."6
- In granite, the models Snelling and Woodmorappe cite "assume that an initially-impermeable granite does not become appreciably permeable until it cools below about 360 °C".3 Lister's estimate, as Cathles reports it, is that "The rate of advance of the cracking front is rapid, about 30 m/year."7
- In the middle crust, where Snelling's granite water must travel to heat a metamorphic belt, Ingebritsen and Manning's fit to measured permeabilities gives a mean of 1.7 × 10⁻¹⁸ m² at 15 km, and their fit to the highest transient values ever inferred gives 5.5 × 10⁻¹⁶ m².88
Where a child gives a distance and a front speed, the requirement is a division.
| Body | Distance the front must cross | Front speed for one year | Front speed found |
|---|---|---|---|
| Devils Tower, jointed section | 90 to 125 m | 90 to 125 m a year | 2.8 to 5.5 m a year, from column width |
| Snelling and Woodmorappe's batholith, from each face | 8,250 m | 8,250 m a year | about 30 m a year, Lister's estimate |
The first row is the Devils Tower article's 16 to 45 years, and the second is the granite article's 275 years. No young-earth paper in any child gives a speed for this front. Snelling and Woodmorappe named it as work to be done in 1998,3 and none of the children found anyone who has done it since.
Global heat is small, regional heat is not
Two children tell skeptics not to lead with the global heat, and the numbers show why. The shares in the third column are this overview's division of each child's figure by Worraker's ocean-floor heat.42
| Rock body | Heat to remove | Share of the 1.4 × 10²⁹ J ocean-floor heat | Power if released in one year |
|---|---|---|---|
| Columbia River basalts | 8.7 × 10²³ J | 6 × 10⁻⁶ | 131,000 W/m² over 210,000 km² |
| California arc granite | 1.7 × 10²⁴ J | about 1 × 10⁻⁵ | 105 W/m² over the whole Earth |
| Barrovian type area, scale only | 1.2 × 10²² J | about 9 × 10⁻⁸ | 2.1 × 10⁵ W/m² over 1,800 km² |
| Every large igneous province, Worraker's total | not exceeding 4.0 × 10²⁶ J | about 3 × 10⁻³ | not given |
Worraker states both halves himself: the total is "insignificant" beside the ocean floor, and the local impact "would have been highly dramatic in the absence of some special, hitherto unrecognized, cooling mechanism."15 The regional figures are about 100 to 160 times the sunlight reaching the top of the atmosphere, held for a year over a plateau or a mountain belt. The granite figure is spread over the whole planet, so it hides a regional load that the granite article does not compute. The heat bites one region at a time, and how fast a region can shed heat is a rate.
Accelerated decay adds heat where the cooling is needed
The polonium argument needs accelerated decay as a clock. The fully formed uranium halos beside the polonium halos imply, in Snelling and Armitage's words, "at least 100 million years worth (at today's rates) of accelerated radioactive decay"18 in the granite whose halos then need it below about 150 °C within days. The metamorphic article prices that much decay as a heat source. Ryan and Dewey's rate for the Dalradian's own potassium, uranium and thorium is "17.5 - 30.0 °K.my⁻¹,"43 so 100 million years' worth, deposited before any of it escapes, is 1,750 to 3,000 K. That rate is for a Scottish metasediment, and no child computes it for a granite, so it is used here for scale only. In the same RATE volume, Humphreys' helium chapter allows the Fenton Hill granodiorite about "90 °C above today's temperature" for a one-year heat pulse.44 The granite article counts three thermal histories for granite in one year, in adjacent chapters of one book.
So the mechanism that makes the halos fast also heats the rock that the halos say cooled in days. Snelling states the cost in 2005 and in 2023.219 No child found a young-earth paper that computes the decay heat inside a pluton during the Flood year, and the whole-Earth version is the subject of The Heat Problem.
The rocks keep their own clocks, and they read in order
Every child that dates a body finds its clocks in an order that a one-year history would erase. Zircon ages in the Tuolumne suite fall in map order, with error bars one to two orders of magnitude finer than the spread.25 Helium ages in Sierra Nevada apatite run 40 to 85 million years45 in granite that crystallised at 125 to 80.45 Snelling himself reports Cooma's mainstream history, built from four clocks with different closure temperatures: "the granodiorite and metamorphic complex supposedly took 45 million years to cool from 735 to 150 °C."9 The flood-basalt article's four clocks are of four kinds, uranium-lead in zircon, paleomagnetic directions, counted laminae and soils, and only one is radiometric.464733 Devils Tower's clock is the width of its columns, measured with a tape.
The order matters more than the ages. A speed-up of decay that scaled every clock by the same factor would keep the order and the spread, and a body built in a year would still come out at one age. The young-earth reply, that different decay systems sped up by different factors, has to predict the observed order, and the granite and metamorphic articles found no model that does.
What the young-earth side gets right, in every child
- Granite magma rises and is emplaced fast, and plutons fill in increments: "large plutons could be filled on time scales of 10¹–10⁴ yr".25
- Single lava flows are built in months to years, and the Roza flow field in about 14 years.
- Metamorphic reactions run in days once the temperature is reached, as Wise said in 1986.
- Water quenched the flood-basalt interiors and circulated through cooling granite, and it does cool rock faster than conduction.
- No exposure age has been measured for Devils Tower, and the mainstream figure has been quoted at 40 million, then 1 to 2 million, then 5 to 10 million years.
- Polonium halos are real and uranium-free, and Gentry's ring measurements are good physics.
- Snelling and Woodmorappe read Cathles' cooling chart correctly.
The children also correct the critics. A skeptic who says the global heat of flood basalts or granite alone disproves the Flood overstates it. A skeptic who says plutons take hundreds of millions of years to cool overstates it too: Cathles' ceiling for any intrusion within 5 km of the surface is 4 million years.7 The honest mainstream numbers are large enough without inflation.
Part 9: Where two articles disagree
The children agree on every number they share. Three use Jaeger's 0.016 D² coefficient, two use Worraker's 1.4 × 10²⁹ J, two use the 28 to 70 darcies, and three trace the 6 to 10 days to the same radiohalo argument. They disagree on two points, both raised by the Devils Tower article about its siblings' material.
How much does water speed up cooling?
The Devils Tower article answers the objection that water cooled the Tower by saying that the granite article "prices hydrothermal cooling with Cathles' and Lister's numbers at a factor of tens over conduction at best." The granite article says something larger. Cathles' own worked example falls from "about 100,000 years" by conduction to "about 20,000 years" at 0.25 millidarcies and about 5,000 at 1 millidarcy,7 a factor of twenty. Snelling and Woodmorappe's rescaling of the same chart falls from about 3 million years to 3,000 at 10 millidarcies,3 and the granite article, answering the objection that water cools rock orders of magnitude faster than conduction, begins: "Granted, and its size is known." A factor of a thousand is what it grants.
So the granite article's figure stands, and the Devils Tower sentence understates it by up to fifty times. The Tower's verdict does not change, because it does not rest on conduction. It rests on the width of the columns, and Goehring and Morris calibrated that relation on lava cooled with water in its cracks. Scaling that article's own figure of about 8 cm for a one-year crossing, a Tower cooled a thousand times faster than conduction would have columns of roughly 8 to 40 cm, not 2 to 3 m. What does change is how the Tower's conduction figures may be used: divided by a thousand, 1,000 to 5,000 years becomes one to five, so conduction alone does not exclude a fast water route. The columns do.
Does fast cooling make disorderly joints?
Tim Clarey writes that "Fast cooling makes less orderly fracture patterns" and points to the disorganised base of Devils Tower.16 The Devils Tower article replies that "Nothing in the measurement literature says so," and cites Li's field test: "cooling processes (slower or faster cooling rate) not affect the ordering behavior."48 The flood-basalt article quotes a paper that does say so, for basalt quenched by water. Long and Wood define entablature, the water-quenched interior of a Columbia River flow, as the part with "smaller column diameters and more irregular pattern fractures than those of colonnade."6
So the literature is split. Long and Wood pair fast water quenching with narrower and less regular columns in basalt; Li finds no effect of cooling rate on regularity in intermediate and felsic lavas. Clarey's general sentence has partial support, and the Devils Tower article's blanket denial goes too far. Its conclusion about the Tower survives, because the Tower's base is the opposite of an entablature. Robinson mapped it as rock that is "massive and jointing, poorly developed. Here the joints form large irregularly shaped blocks rather than columns."49 A water quench of the kind Long and Wood describe makes small columns. Large blocks with poorly developed joints are what the width rule predicts for the slowest-cooled part of a body, and in Závada's model the base sits over the feeding conduit, the last part of the body to cool.
Objections and responses
"Each article chose the slowest mechanism to make the Flood look bad." The reverse. Each child grants the fastest published route before pricing it: Snelling and Woodmorappe's own 3,000 years, which the granite article says is read correctly; Goehring and Morris's relation with water in the cracks; Thordarson and Self's 14 years for the whole Roza flow field; Ague and Baxter's 200,000-year thermal peak; Snelling and Armitage's own fluid-transport model for the halos. Where a child prices a route that no young-earth author proposes, such as friction in the metamorphic article, it says so.
"The heat was removed by a miracle, and physics cannot refute a miracle." That is true, and the granite article grants it. Two things follow for the whole group. The heat of these rocks is small beside the ocean-floor heat, so a miracle that removes the larger heat removes this one without noticing. But a miraculous cooling stops the thermal literature and the halos from being evidence of a natural fast cooling, and the young-earth papers in these articles cite Cathles, Petford, water-quenched entablature and the radiohalos as though physics did the work. The two arguments cannot both be used.
"All these ages assume constant decay rates." The arguments do not need the ages. They need the order and the spread, which a uniform speed-up keeps, and most of the clocks are not radiometric at all. Column width is measured with a tape. Conduction uses laboratory constants. Soils, roots, counted laminae and paleomagnetic directions involve no decay. Ague and Baxter's 200,000 years comes from diffusion in apatite and garnet, with laboratory coefficients, and the metamorphic article notes that the fast and slow results come from the same methods.
"Mainstream geologists disagree among themselves, about rapid metamorphism, the Deccan pulses and the shape of Devils Tower." They do, and each dispute is far from a year. The Barrovian heat dispute is between about 20 million years and about 200,000. The Deccan dispute is between steady and pulsed eruption over about a million years. The Devils Tower dispute is between a coulée cooling in about 4,000 years and a sheet solidifying in about 1,000. The nearest end of every dispute is at least a thousand Flood years.
"Put these rocks after the Flood." This is the strongest move available, and Austin makes it for the flood basalts. It works for the year. Its cost is that the rocks stop being Flood evidence, and that the soils, lakes and cooling times have to fit into a post-Flood interval that nobody has stated. The same move is harder for bodies that the young-earth authors themselves tie to the Flood: Clarey's Devils Tower formed in the receding phase and was stripped by the draining water, and Snelling's Cooma was made by Flood granites. Gentry's older version, created Precambrian granites, runs into Henke's point that "Precambrian granites have much the same mineralogies, textures and structures as Cretaceous and other Phanerozoic granites".50
"The batholiths did not need to be cold by the end of the Flood." That is Snelling and Woodmorappe's own position, and it is an honest one.3 It moves the problem from the Flood year to the roughly 4,500 years since, and the granite article's 10⁴ to 10⁷ years is still longer than that. It cannot help a body that had to be cool and jointed before the receding water stripped its cover, which is the Devils Tower case and the "emplaced, cooled, and unroofed" claim in Walker 2003.10 And Snelling's later 6 to 10 days gives the position up.
"Catastrophic plate tectonics makes everything faster." It makes burial, subduction and exhumation faster, and Oard argues it raises pressure at shallow depth. None of these changes how fast heat conducts or how permeable rock is. The metamorphic article finds that overpressure cuts an inferred depth by at most a factor of two and cuts no temperature. Catastrophic plate tectonics adds heat; it does not remove any.
Skeptic: "The heat alone disproves the Flood." Not globally. The Columbia River basalts would warm the ocean by 0.16 K, and one arc of granite released in a year is about 105 W/m² over the planet. Both children say the global argument overstates the case. The fair objections are the regional power and the rates, and they are enough.
"The polonium halos are only one argument. The cooling case does not depend on them." For the Flood year it does. The 6 to 10 days for granite and the 12 to 20 days for Cooma trace to the halos, and the only other figure inside a year, Walker's "couple of months," cites a paper that says 3,000 years. Without them the young-earth literature's only thermal number for these rocks is 3,000 years, and its authors decline to claim that it fits inside the Flood.
Issues and unanswered questions
- No young-earth thermal calculation reaches a Flood year for any of the five bodies. Snelling and Woodmorappe 1998 is the only thermal model, and it gives 3,000 years to the 75 per cent mark. Devils Tower and the flood basalts have no young-earth cooling time at all.
- The speed of the cracking front under Flood conditions has never been computed. It is the number that would decide the water route in granite, in lava and, through the crust, in metamorphic belts. Snelling and Woodmorappe asked for it in 1998.
- The decay heat inside a pluton during the Flood year has not been computed by anyone. Part 8 uses the Dalradian rate for scale only. The Heat Problem carries the global budget.
- Cheap measurements would settle several open points. A beryllium-10 exposure age on Devils Tower and its largest talus blocks. Brawley's photometric test on existing halo slides. One independent thermometer traverse across a Barrovian isograd. Ship Rock, with a kilometre of removed cover, has no young-earth treatment at all.
- Several sources the children needed were not obtained. Laney and Laughlin's depth-temperature table, on which the 150 °C annealing ceiling rests; Feather 1978, the one claim that could break the halo census; the body of Long and Wood 1986, with its computed entablature cooling times; Clemens 2005, the source of the creationists' 30,000 years; England and Thompson 1984; and Reidel's whole-province count of Columbia River interbeds. Each child lists its own.
- The young-earth literature has not chosen when the flood basalts erupted. Until it does, they are either a Flood deposit that fails the year or a post-Flood deposit whose duration is unstated.
- Part 9 corrects two statements in the Devils Tower article. Its account of the granite article's hydrothermal factor is too small, and its denial that any measurement links fast cooling to irregular joints is too broad. Neither changes its verdict.
Verdict
The young-earth models are right about speed wherever speed can be watched or reproduced. Magma rises fast, plutons fill in increments, a flood-basalt flow is built in years, metamorphic reactions run in days, and water does cool rock faster than conduction. They are also right that the global heat of these rocks is small beside the ocean-floor heat they already face.
They have not shown that the rocks could cool, or be heated, inside the year. Conduction takes 10⁵ to 10⁷ years for a batholith and over a million for a metamorphic belt. Water helps only behind a cracking front that moves metres to tens of metres a year, through crust thousands of times too tight. Devils Tower's columns read decades at the fastest. The flood basalts hold soils, a counted lake and eggshells between their flows. The clocks inside the rocks read in an order that a one-year history would erase. Against all of this the young-earth literature offers one thermal model, which gives 3,000 years and declines to claim the Flood, and one short figure, 6 to 10 days, which comes from polonium halos that record dose rather than time. On the evidence the five children assembled, the igneous and metamorphic rocks placed in the Flood year could not have cooled, or been heated, inside that year. The most open point left, the Devils Tower exposure age, is one measurement away from an answer.
Sources
- 1.
Wise, Kurt P. “How Fast Do Rocks Form?” Proceedings of the First International Conference on Creationism 2:197–203. Creation Science Fellowship, Pittsburgh. 1986. A paper in the proceedings of the First International Conference on Creationism, a creationist meeting, on the speed at which rocks form. The article uses it for Wise's statement that heating buried sediment would take many millions of years, and for his point that the objections to creationism come from regional metamorphism.
- 1a.
Page 199: “The biggest problem, however, lies again in the problem of heat. Rapid burial beneath many kilometers of sediment produces instantaneous pressure increases, but once again it takes too much time to heat the sediment. In fact it would take many millions of years to heat up sediment buried 20 kilometers beneath the surface.” ↩ ↩
- 1b.
Page 198: “It seems that any metamorphic reaction can be reproduced in the lab. Each of these reactions can be made to occur in less than a few weeks. The higher the temperature and/or pressure, the faster the reaction. It turns out that any reaction which involves more than about 300 degrees Centigrade can be reproduced in the course of a single day or less. Chemical equilibrium in the process of metamorphism is thus rather quickly reached once the thermal conditions are achieved. It is, however, rather difficult to achieve those conditions.” ↩
- 1a.
- 2.
Snelling, Andrew A. “Radiohalos in Granites: Evidence for Accelerated Nuclear Decay.” Radioisotopes and the Age of the Earth, Volume II, 101–207. Institute for Creation Research (El Cajon) and Creation Research Society (Chino Valley). Edited by L. Vardiman, A. A. Snelling and E. F. Chaffin. 2005. Chapter 3 of a 2005 young-earth creationist research volume, in which Andrew A. Snelling of the Institute for Creation Research studies polonium and uranium radiohalos, the concentric darkened shells that alpha particles leave around tiny crystals in biotite, a black mica. Its abstract concludes that granite plutons, large underground bodies of granite, cooled within 6 to 10 days, and that radioisotope decay must have been accelerated to form the uranium radiohalos. The article uses it as the source of its 6 to 10 day cooling claim.
- 2a.
Page 145, section § 6.7 "The Heat Problem": “Convective flows of hydrothermal fluids might be capable of moving and dissipating heat from granitic plutons, but an additional, as yet unknown mechanism would have been needed to remove the heat generated by the accelerated radioisotope decay.” ↩ ↩ ↩ ↩
- 2b.
Page 147: “the timescale for the cooling of granitic plutons was extremely short, calculated at between six and ten days. And it should be noted that this timescale is constrained by the half-lives of these isotopes, and not by the assumption that these granites formed during the Flood year.” ↩ ↩
- 2a.
- 3.
Snelling, Andrew A., and John Woodmorappe. “The Cooling of Thick Igneous Bodies on a Young Earth.” Proceedings of the Fourth International Conference on Creationism, 527–545. Pittsburgh: Creation Science Fellowship. Edited by R. E. Walsh. 1998. A creationist paper presented at the Fourth International Conference on Creationism in 1998, by Andrew Snelling, of Answers in Genesis, and John Woodmorappe. It argues that water moving through cracks in a cooling pluton can cool a batholith in about 3,000 years, and the article treats it as the only young-earth thermal model of a batholith. Its page numbers are those of ICR's 17-page reprint, not the original pages 527–545.
- 3a.
Page 6: “An infinitely-long batholith that is 11 km wide, 16.5 km thick, and is buried 20 km below the surface of the ground, when at zero rock permeability (that is, conductive cooling only) needs a few million years to cool. But with the intensity of convective cooling that is allowed by a permeability K of 10 millidarcies (easily exceeded—see below), the time to cool this batholith falls to a mere 3,000 years.” ↩ ↩ ↩
- 3b.
Page 6: “the cooling in Figure 3 starts with solidus temperatures and ends at 25% of the difference between ambient temperatures and solidus temperature. The remainder of the cooling to ambient crustal temperatures is not covered by Figure 3 …” ↩
- 3c.
Page 7: “Thus far, we have discussed long-inert granites. By contrast, the permeability of a granite in the actual process of cooling remains unknown. The most recent models (Ingebritsen & Hayba, 1994) assume that an initially-impermeable granite does not become appreciably permeable until it cools below about 360 °C, at which time its ductile behavior gives way to brittle behavior, and thus jointing becomes possible.” ↩ ↩
- 3d.
Page 7: “These rates of repeated creation of joints (under catastrophic tectonism) and the opposing rates of 'healing' in still-ductile rock need to be quantified.” ↩ ↩
- 3e.
Page 6: “This discussion does not imply that all of the large batholiths had cooled by the time they were uplifted after the Flood.” ↩ ↩
- 3a.
- 4.
Snelling, Andrew A. “Radiohalos: Startling evidence of catastrophic geologic processes on a young earth.” Creation Ministries International. Apr 5, 2007. A popular article for general readers, with photographs of uranium and polonium halos in granite. It argues that the polonium halos show granites solidified and cooled in just 6 to 10 days, and that uranium decayed up to a billion times faster in the past; it cites Laney and Laughlin's 1981 study for the 150 °C annealing ceiling. The article uses it as the plain-language version of the RATE argument.
- 4a.
“In other words, the radioactive decay of uranium was formerly up to a billion times faster than it is today!” “polonium halos mean that the granites solidified and cooled in just 6 to 10 days!” The same passage requires that the polonium. “all had to concentrate within hours, or a few days at the most.” ↩ ↩
- 4a.
- 5.
Lamur, Anthony et al. “Disclosing the temperature of columnar jointing in lavas.” Nature Communications 9:1432. 2018. A laboratory study by seven authors of basalt from Eyjafjallajökull volcano in Iceland as it cooled. It found that stress built up and the rock failed between 890 and 840 °C, below the solidus (the temperature below which the rock is fully solid, here 980 °C), and that this window held whatever the imposed cooling rate. The article uses it because the window stays put whatever the cooling rate, which leaves column width as the only variable that can record the rate.
- 6.
Long, Philip E., and Bernard J. Wood. “Structures, textures, and cooling histories of Columbia River basalt flows.” Geological Society of America Bulletin 97(9):1144–1155. Sep 1986. A research paper on the structures, textures and cooling histories of Columbia River basalt flows. Entablature is the zone of small, irregular columns in the middle of a thick flow. The article uses it for two points: ordinary heavy rain cannot make entablature, so standing or flooding water is needed, and that water follows the cooling lava down rather than racing ahead of it.
- 6a.
Section Abstract: “We have found that a water infiltration front can explain the presence of a thick, quenched, flow interior, provided that the infiltration front moves downward just behind the lava solidification front.” ↩ ↩
- 6b.
Section Abstract: “The colonnade refers to the well-defined columnar structure of many flows, which appears in the lowermost 10% to 30% and, in places, the uppermost 10% to 20%. Entablature refers to those parts of a flow that have smaller column diameters and more irregular pattern fractures than those of colonnade. Entablature commonly occupies the central 60% to 70% of a flow.” ↩
- 6a.
- 7.
Cathles, Lawrence M. “Fluid Flow and Genesis of Hydrothermal Ore Deposits.” Economic Geology Seventy-Fifth Anniversary Volume, 1905–1980, 424–457. El Paso: Economic Geology Publishing Co. Edited by Brian J. Skinner. 1981. A chapter in a 1981 anniversary volume of Economic Geology, with a chart (its Figure 6) and worked examples of how fast an intrusion cools by conduction and by ground-water convection. Figure 6 is the source of the chart that Snelling and Woodmorappe use as their Figure 3, and the article checks their numbers against it.
- 7a.
Page 440: “Lister (1974) has pointed out that the permeability of a cooling intrusion can be very high due to the magnitude of thermal contraction which will occur in cooling assisted by pore fluid convection and the extent of thermal cracking expected. Lister has estimated that intrusion permeabilities of about 10 darcies may occur after thermal cracking by interaction with ground water but before substantial sealing by mineral deposition, static fatigue, or collapse. After static fatigue and collapse, the permeability may be reduced to a few millidarcies. The rate of advance of the cracking front is rapid, about 30 m/year.” ↩ ↩
- 7b.
Page 440: “The precise location of this upper bound (which depends most strongly on the chosen value of thermal diffusivity and here is about 4 m.y.) is not so important as the recognition that, for a limited depth range, an upper bound must exist. For the conductivities chosen here, no 800 °C intrusion, no matter how large, can maintain against conduction an anomaly greater than 200 °C within 5 km of the surface for more than 4 m.y.” ↩ ↩
- 7c.
Page 440: “Figure 6 shows that a dikelike plutonic intrusion 2 km wide, 3 km high, whose top is 3.66 km below the surface, will take about 100,000 years to reduce its temperature contrast relative to ambient at the time of intrusion to 25 percent its initial value if the intrusion and the rock it intrudes have zero permeability and cooling is entirely by conduction. If the intrusion and intruded rock have a permeability of 0.25 millidarcies, cooling time will be about 20,000 years. If the permeability of intrusion and host is 1 millidarcy, the time will be about 5,000 years.” ↩
- 7a.
- 8.
Ingebritsen, Steven E., and Craig E. Manning. “Permeability of the continental crust: dynamic variations inferred from seismicity and metamorphism.” Geofluids 10(1–2):193–205. 2010. A review of how easily fluid moves through rock, which is permeability, in the continental crust, using geothermal data and the progress of metamorphic reactions driven by fluid flow. It finds that mean permeability in tectonically active crust falls with depth, and that the higher transient values inferred from seismicity and metamorphism follow a curve of the same form, shifted to higher permeability at a given depth. The article uses the mean curve and the transient curve to test whether hot water could carry enough heat to the depth of a metamorphic belt.
- 8a.
Page 193, section Abstract: “Compilation of such data yields a fit to these elevated, transient values of log k ≈ −11.5 − 3.2 log z, suggesting a functional form similar to that of tectonically active crust, but shifted to higher permeability at a given depth.” ↩ ↩
- 8b.
Page 193, section Abstract: “Geothermal and metamorphic data combine to indicate that mean permeability (k) of tectonically active continental crust decreases with depth (z) according to log k ≈ −14 − 3.2 log z, where k is in m² and z in km.” ↩ ↩
- 8a.
- 9.
Snelling, Andrew A. “Radiohalos in the Cooma Metamorphic Complex, New South Wales, Australia: The Mode and Rate of Regional Metamorphism.” Proceedings of the Sixth International Conference on Creationism, 371–387. Creation Science Fellowship and Institute for Creation Research. Edited by A. A. Snelling. 2008. A 2008 conference paper by Andrew Snelling, then Director of Research at Answers in Genesis, a creationist organisation. It counts polonium radiohalos in rock samples along a line from low-grade schists to high-grade gneisses and the central granodiorite, and finds the counts rise with metamorphic grade. It attributes them to hot fluids from the cooling granite and claims the whole complex formed in 12–20 days, which the article treats as the only time estimate a young-earth author gives for a regional metamorphic terrane.
- 9a.
Page 371, section Abstract: “Furthermore, generation of the regional metamorphic complex only required 12–20 days, based on the catastrophic granite formation of the adjacent Murrumbidgee Batholith whose heat and hydrothermal fluids generated the regional metamorphic zones of the complex from the mineral constituents of the original fossiliferous sediment layers, then the central granodiorite as a consequence.” ↩ ↩
- 9b.
Page 379: On Gentry's created-granite model. “Such an interpretation is inconsistent with the field and petrological evidence from the Cooma metamorphic complex and the Cooma granodiorite. The granodiorite is in fact the product of the regional metamorphism of the fossiliferous (Flood-deposited) sedimentary rocks that host the granodiorite …” ↩
- 9c.
Page 384: “According to this curve, the granodiorite and metamorphic complex supposedly took 45 million years to cool from 735 to 150 °C. However, if as has been shown from several lines of evidence, radioisotope decay rates were grossly accelerated during the Flood event (Vardiman, Snelling, & Chaffin, 2005), while catastrophic plate tectonics were operating to produce catastrophic granite formation, then this cooling would have occurred within days”. ↩
- 9a.
- 10.
Walker, Tas. “Granite grain size: not a problem for rapid cooling of plutons.” TJ (Journal of Creation) 17(2):49–55. 2003. A 2003 article by the creationist Tas Walker in the creationist journal TJ (Journal of Creation). It argues that coarse grain in granite does not show slow cooling, because crystal size depends on more than the cooling rate, and that water explains the rapid cooling of plutons. The article uses it for the field examples it grants and for how Walker describes the Snelling and Woodmorappe answer.
- 11.
Snelling, Andrew A. “Towards a Creationist Explanation of Regional Metamorphism.” Creation Ex Nihilo Technical Journal 8(1):51–77. 1994. A 1994 paper in a creationist technical journal, by a geologist who proposes a creationist explanation of regional metamorphism. It argues that the mineral zones formed from the original sediment at only moderate temperatures and pressures, and that catastrophic burial and volcanic heat during the Flood could have produced them. The article calls it Snelling's founding paper on the subject, and uses it for his statement of the mainstream model and his concession that heat is the biggest problem for creationists.
- 11a.
Page 72: “As was noted at the outset, the biggest problem creationists face with the conventional scenario for regional metamorphism is the heat presumed to have been involved, given that even with rapid burial beneath kilometres of sediments time is needed to produce that heat within the sediment pile.” ↩
- 11b.
Pages 72–73: The sentence turns the page. “the evidence presented now indicates that composition is the primary factor in metamorphism”. “we have now seen that only moderate temperatures may be needed to transform the precursors into the index minerals of the zones of regional metamorphism, and such moderate temperatures would have conceivably been generated in the short time-scale in the Flood event described above, both due to the thicknesses of the sediment piles catastrophically accumulated, and due to the increased heat flow from the mantle because of rapid plate tectonics.” ↩
- 11a.
- 12.
Austin, Steven A. et al. “Catastrophic Plate Tectonics: A Global Flood Model of Earth History.” Proceedings of the Third International Conference on Creationism, 609–621. 1994. A 1994 conference paper by six authors that presents catastrophic plate tectonics, a global Flood model of earth history. The article uses it because its predictions section says Flood models claim to explain regional metamorphism, and cites Snelling's two 1994 papers for that claim.
- 12a.
Section Conclusion, "Predictions": “Since Flood models are usually tied to young-earth creationism, they also claim that it is possible on a short timescale to explain the cooling of plutons and ocean plate material; regional metamorphism (see, for example, Snelling);”. The passage cites the two 1994 Snelling papers. ↩
- 12a.
- 13.
Baumgardner, John. “101 Questions and Answers Concerning Catastrophic Plate Tectonics.” globalflood.org. Apr 2012. Answers by Baumgardner, who represented the catastrophic plate tectonics model in a peer review of Flood models that ran from early 2009 to the summer of 2011. The review was run by In Jesus' Name Productions, a Christian film ministry, and each panelist put written questions to each model's author. The article uses it because it treats the Franciscan blueschists of California as support for catastrophic plate tectonics.
- 13a.
Section Question 4: “This difficulty, of course, disappears in the CPT framework because the subduction and exhumation velocities are orders of magnitude higher and the time scale is orders of magnitude shorter.” ↩
- 13a.
- 14.
Oard, Michael J. “Metamorphic rocks can form at shallow depths.” Journal of Creation 29(2):13–15. 2015. A short Perspectives article in the creationist Journal of Creation. It reviews laboratory evidence that rocks form across a wide range of pressures and temperatures, then argues that stress from plate movement could let ultrahigh-pressure minerals form at less than half the depth usually assumed, possibly less than 50 km. The article uses it because the author argues that directed stress, not the weight of overlying rock, could drive the reactions, so a pressure does not fix a depth.
- 14a.
Page 15: “In the CPT model, plate movements of metres per second have the capability to create greater tectonic pressure at shallow depths and provide a better explanation of zones of UHPm. … As a result we are in a better position to explain how UHPm formed, possibly at depths shallower than 50 km.” ↩
- 14a.
- 15.
Worraker, William J. “Heat Problems Associated with Genesis Flood Models—Part 4: Heat Deposited by Magmatic Activity.” Answers Research Journal 16:201–251. 2023. A paper by a young-earth physicist in the Answers Research Journal on the heat that large igneous provinces (continental flood basalts and oceanic LIPs) deposit as they erupt, set against the heat that Genesis Flood models must remove. It gives the heat needed to form new ocean floor under catastrophic plate tectonics as 1.4 × 10²⁹ J, derived from Furlong and Chapman's ~3.9 × 10¹⁴ J/m². The article takes that 1.4 × 10²⁹ J figure as the heat catastrophic plate tectonics must remove, and it quotes the paper's view that the basalts' heat is small beside it.
- 15a.
Page 221: “Although continental flood basalt provinces (CFBs) are more accessible to geological investigation than oceanic LIPs, the heat deposited in their formation is difficult to estimate because the total emplaced volume is often highly uncertain. … the total amount of heat involved (not exceeding 4.0 × 10²⁶ J) is insignificant in comparison with the heat deposition involved in forming the ocean floors (1.4 × 10²⁹ J). Thus the heat released in the formation of LIPs adds relatively little to the overall problem of discerning the mechanism whereby the ocean floors must have cooled during and after the Flood. However, the local impact of the heat from LIPs, which in many cases must have been released within a matter of days or weeks at most, would have been highly dramatic in the absence of some special, hitherto unrecognized, cooling mechanism.” ↩ ↩
- 15a.
- 16.
Clarey, Tim. “Devils Tower: Mysterious Columns and Engineered Lichens.” Acts & Facts. Institute for Creation Research. Feb 28, 2023. A short article in Acts & Facts, the magazine of the Institute for Creation Research. It argues that the Tower formed during the receding phase of the Flood and was exposed about 4,500 years ago as the floodwaters drained, and it says that fast cooling makes less orderly fracture patterns. The article uses it as the young-earth account of the Tower's cooling and exposure, and tests its claims against the mainstream evidence.
- 16a.
Section Columns from Cooling, paragraph 1: “Studies suggest all of these columns cool from the top, with contraction forming regularly spaced fractures that propagate downward. During the Flood, groundwater percolating along the open fractures likely caused the lower part of the magma to cool quickly. Fast cooling makes less orderly fracture patterns. We see this at the base of the tower where the columns become chaotic and disorganized.” ↩ ↩
- 16b.
Section Columns from Cooling, paragraph 2: “ICR scientists determined that these magmas formed during the receding phase of the Flood after most of the sediments were deposited.” ↩
- 16c.
Section Why Devils Tower Is Young, paragraph 2: “But if Devils Tower was exposed 5 to 10 million years ago, as conventional scientists claim, it probably would have completely eroded away in this amount of time. At the very least, it should be entirely buried in its own debris of broken columns. And the Belle Fourche River doesn't seem to be eroding away any broken columns since none are found within its waterway. The relatively thin buildup of broken columns at the tower's base fits its recent exposure 4,500 years ago during the draining of the floodwaters.” ↩
- 16a.
- 17.
Clarey, Tim. “Entablature Reveals Flooding of Columbia River Basalts.” Institute for Creation Research. Oct 31, 2022. A short article on the website of the Institute for Creation Research by Tim Clarey, a research scientist there who holds a Ph.D. in geology. It argues that entablature, the irregular, wavy-fractured texture that makes up most of the Columbia Plateau lavas, forms when floodwater runs over a lava that has begun to cool. The article calls it the strongest creationist observation about the basalts, and it places Clarey among the creationists who put the lavas inside the Flood's receding phase.
- 17a.
“Flood geologists have a better explanation. The Columbia Plateau lavas erupted near the end of the Flood's receding phase (Miocene). Floodwater likely hadn't fully drained from the region, and rapid creation of new ocean crust was ongoing, resulting in large earthquakes and tsunamis. These massive waves were still crashing across Oregon and Washington and over the tops of the fresh lava flows, quenching the molten centers and forming entablature.” ↩ ↩
- 17a.
- 18.
Snelling, Andrew A., and Mark H. Armitage. “Radiohalos—A Tale of Three Granitic Plutons.” Proceedings of the Fifth International Conference on Creationism, 243–267. Creation Science Fellowship, Pittsburgh. Edited by R. L. Ivey. 2003. A conference paper, given in August 2003, that scanned biotite from three granite plutons (large bodies of cooled magma) for radiohalos. Its abstract argues that the polonium halos were formed by hot fluids moving through the rock, and that neither they nor the granites could have been created all at once in finished form (fiat creation). The article uses it as the young-earth movement's own 2003 rejection of Gentry's primordial model, in which the polonium was present from creation and was not produced by uranium decay.
- 18a.
Section Abstract: “the observed fully-formed ²³⁸U and ²³²Th radiohalos imply at least 100 million years worth (at today's rates) of accelerated radioactive decay has occurred.” ↩ ↩
- 18b.
Table 1, page 11: Column totals over 19 samples and 895 slides: ²¹⁰Po 1,857; ²¹⁴Po 152; ²¹⁸Po 2; ²³⁸U 559; ²³²Th 37. Both ²¹⁸Po halos are from sample SMG-5, Stone Mountain. The text gives the ratio of ²¹⁰Po to ²¹⁴Po halos as. “to a high of 69 ²¹⁰Po halos for every ²¹⁴Po radiohalo”. and about nine to one in the Cooma granodiorite. The paper's text and its table disagree on two subtotals: the text gives 1139 ²¹⁰Po radiohalos for the Stone Mountain samples where the table sums to 1,109, and 437 for La Posta where the table sums to 443. The figures used here are the table's. ↩
- 18c.
Page 13: “the hypothesis that the three different types of Po radiohalos found in biotites always represent the decay of primordial Po (original Po not derived by U-decay) (Gentry, 1979, 1980, 1982, 1983, 1984, 1986, 1988, 1993) has been falsified”. ↩
- 18a.
- 19.
Snelling, Andrew A. “Radiohalos through earth history — What clues can they provide us?” Proceedings of the Ninth International Conference on Creationism, 540–560. Cedarville University. Edited by J. H. Whitmore. 2023. A paper for a creationist conference, by Andrew Snelling of Answers in Genesis. It counts radiohalos, the tiny darkened rings that alpha particles from uranium decay leave around a zircon grain in biotite (a black mica), in 147 granites and regional metamorphic rocks dated 33 to 3200 million years old. It argues that the halos are likely due to accelerated uranium decay during the Flood, and that 100 million years' worth of that decay at today's rate is needed to make good visible halos. The article uses it as the most recent young-earth statement on the heat problem.
- 19a.
Page 544: “Hundreds of millions of years' worth of ²³⁸U decay must have occurred within days so enough daughter Po isotopes were produced rapidly to be transported by hydrothermal fluids to closely adjacent locations within the host crystals to form separate ('orphan') Po radiohalos (Snelling 2005a). One major objection raised is the huge amount of heat (as well as radiation) that would seem to be generated by the pulse of accelerated ²³⁸U decay.” ↩ ↩
- 19a.
- 20.
Austin, Steven A. “The Declining Power of Post-Flood Volcanoes.” Acts & Facts 27(8). Aug 1, 1998. A magazine article by a creationist writer, printed in Acts & Facts, which the Institute for Creation Research publishes. The article uses it as the creationist source for placing the basalts in a post-Flood decline of volcanic power. The article also says Austin gives the Laki figures accurately, and that his point that ancient eruptions were about a thousand times bigger than modern ones is correct.
- 20a.
“Thus, energies of ancient lava-flow volcanoes appear to exceed by a thousand times their modern counterparts. Again, this evidence is consistent with the catastrophist interpretation of the declining power with time of post-Flood volcanoes.” ↩
- 20a.
- 21.
Morris, John D. “Were the Huge Columbia River Basalts Formed in the Flood?” Acts & Facts 33(5). Institute for Creation Research. 2004. An article by John D. Morris, published by the Institute for Creation Research, that asks whether the Columbia River basalts were formed in the Flood. It says the eruptions probably came in the last stages of the Flood or in the years of readjustment after it, and it gives the area as 65,000 square miles and the volume as about 40,000 cubic miles. The Flood Basalts article uses it as the creationist answer on timing and as the source of the old volume figure.
- 21a.
“Occurring in layers stratigraphically below the Columbia River Basalts are thick layers of water-deposited, fossil-bearing, sedimentary rock, obviously deposited by the Flood itself. Thus, Flood advocates interpret these mega-eruptions of basalt as probably occurring during the very last stages of the Flood or in the years of readjustment to follow, as Earth's systems regained the relative equilibrium in which we now find them.” ↩
- 21a.
- 22.
Oard, Michael J. “Devils Tower can be explained by floodwater runoff.” Journal of Creation 23(2):124–127. 2009. A journal article whose title states its claim that floodwater runoff can explain Devils Tower. The article uses it for the young-earth argument that Flood runoff stripped the rock around the Tower and that the Tower cannot have stood for millions of years, and it tests that argument.
- 22a.
Page 125: “Devils Tower should have been destroyed quickly, surely in less than 100,000 years.” The preceding block quotation, a recollection of blocks crashing onto the talus in November 1954, is Oard's reference 6, Robinson and Davis 1995, p. 36. ↩
- 22a.
- 23.
Petford, Nick et al. “Granite magma formation, transport and emplacement in the Earth's crust.” Nature 408(6813):669–673. Dec 7, 2000. A review article in Nature that goes through the physical processes that move granite magma from its source, through the crust, to where it is emplaced. It concludes that granite magmatism is dynamic and fast, not the slow, multi-million-year process once assumed. The article uses it as the source that retired the old picture of slow granite magma.
- 23a.
Page 673: “The rate-limiting step in granite magmatism is the timescale of partial melting; the follow-on stages of segregation, ascent and emplacement can be geologically extremely rapid—perhaps even catastrophic.” ↩
- 23a.
- 24.
Jaeger, J. C. “The Temperature in the Neighborhood of a Cooling Intrusive Sheet.” American Journal of Science 255(4):306–318. Apr 1957. A mathematical solution, published in 1957, for how a sheet of magma (a sill or dike) cools by conduction, with the heat released as it solidifies included. Earlier solutions by Lovering and Larsen left that heat out, so the author says their times to solidify must be roughly doubled and their contact temperatures are too low by of the order of 100 °C. The article uses it for the mainstream conduction figure, and the author states that the model assumes conduction alone.
- 24a.
Page 311: “Solidification is complete after 0.016D² years instead of the 0.007D² years found from Larsen's less accurate calculation.” For the granite case, liquidus 700 °C, solidus 500 °C, latent heat 80 cal/g, D in metres. ↩
- 24a.
- 25.
Coleman, Drew S. et al. “Rethinking the emplacement and evolution of zoned plutons: Geochronologic evidence for incremental assembly of the Tuolumne Intrusive Suite, California.” Geology 32(5):433–436. May 2004. A geochronology paper that dates eleven samples from the Tuolumne Intrusive Suite in Yosemite by uranium-lead dating of zircon crystals, to test whether the suite grew from one large magma chamber or from many small intrusions. It concludes that the suite was assembled over at least 10 million years, and that the Half Dome Granodiorite intruded over a period approaching 4 million years. The article uses it for that timescale, which it says the creationist accounts leave out.
- 25a.
Page 433: The abstract: “New U-Pb geochronologic data indicate that the Tuolumne Intrusive Suite, California, was assembled over a period of at least 10 m.y. between 95 and 85 Ma, and that the Half Dome Granodiorite intruded over a period approaching 4 m.y. Simple thermal considerations preclude the possibility that a magma chamber the size of the Half Dome pluton could have existed as a liquid at shallow crustal depths for that long.” ↩
- 25b.
Page 433: “Samples of the Glen Aulin and Kuna Crest plutons yield indistinguishable ages of 93.1 ± 0.1 (Fig. 2A) and 93.5 ± 0.7 Ma (Fig. 2B), respectively,”. and Half Dome Granodiorite samples at the contacts with them. “yield ages of 92.8 ± 0.1”. Ma. Page 434: The same paper gives 91.7 ± 0.2 Ma in Yosemite Valley, 91.1 ± 0.1 Ma at the top of Half Dome, and 88.8 ± 0.8 Ma at the contact with the Cathedral Peak Granodiorite. ↩
- 25c.
Page 433: “large plutons could be filled on time scales of 10¹–10⁴ yr (Clemens and Mawer, 1992; Petford, 1996).” ↩
- 25a.
- 26.
Reiners, Peter W. et al. “Zircon (U-Th)/He thermochronometry: He diffusion and comparisons with ⁴⁰Ar/³⁹Ar dating.” Geochimica et Cosmochimica Acta 68(8):1857–1887. 2004. A laboratory study of how helium escapes from zircon crystals, tested against argon dating of slowly cooled granites. It found that the zircon helium clock closes, meaning it stops losing helium, at about 170 to 190 °C for typical plutonic cooling, and it dated granite from the Speel River pluton, collected at sea level in Tracy Arm of Holkham Bay, about 200 km south of Juneau. The article uses it for the five clocks read from that one granite, sample 8500-15.
- 26a.
Page 1865, section § 3.5 "Tracy Arm/Holkham Bay": “Taken together these data suggest a remarkably smooth hyperbolic cooling history for this sample since crystallization at 60 Ma, with a strong deceleration of cooling between ~45–55 Ma, and final cooling through ~70°C at ~7–8 Ma.” ↩
- 26a.
- 27.
Figures marked † in Part 7, and the conduction, permeability and heat figures in Parts 2, 3 and 8, are the child articles' own arithmetic, not published results, with every input printed there. Granite Cooling works its slab table, its 28 to 70 darcies and its arc heat in its Parts 3, 4 and 6 from Jaeger 1957, Cathles 1981 and Ducea 2001. Metamorphic Rocks prints every input in
conduction-times.ts. Flood Basalts states its textbook inputs for density, specific heat, latent heat and diffusivity in its Parts 2 and 5. Devils Tower's cooling and erosion figures come fromcooling-model.ts. Polonium Radiohalos' supply rate is a round-number estimate in its Part 4. ↩ ↩ - 28.
Ague, Jay J., and Ethan F. Baxter. “Brief thermal pulses during mountain building recorded by Sr diffusion in apatite and multicomponent diffusion in garnet.” Earth and Planetary Science Letters 261(3–4):500–516. 2007. A research paper on the classic Barrovian zones of Scotland, which are rocks of rising metamorphic grade. The authors measured how strontium in apatite and several elements in garnet had spread between the zones of garnet, staurolite and sillimanite, and used how much of that pattern survived to time the heat. They found that the thermal peak lasted a few hundred thousand years, probably moved by magma and fluid rather than slow conduction. The article uses it for the brief peak inside a 10 to 15 million year mountain-building event, and for the method of reading time from a sharp chemical step in a crystal.
- 28a.
Page 512: “While a background (i.e., < ∼500 °C) regional conductive heating and cooling due to overthickening probably spanned nearly the entire 10–15 Ma orogeny, the thermal peak conditions lasted for only 200–300 kyr and were attained c. 465 Ma close to the end of the orogeny (Fig. 10).” ↩
- 28a.
- 29.
Viete, Daniel R., and Gordon S. Lister. “On the significance of short-duration regional metamorphism.” Journal of the Geological Society 174(3):377–392. 2017. A review that defines short-duration regional metamorphism as metamorphism on time scales short enough that its heated zone stays much thinner than the crust: under about 10 million years in a mountain-building crust, or under about 5 million years where oceanic lithosphere is pushed beneath another plate. It says that thermal models cannot reach the peak temperatures of mountain-building collisions and subduction without exceptional heat sources, and that diffusion geospeedometry, which typically gives durations under 1 million years, must be checked by benchmarking the new high-precision petrochronology techniques against those results. The article uses it for that definition and for the field's own doubt about the shortest durations.
- 29a.
Section Abstract: “Short-duration regional metamorphism is a recently observed and poorly understood phenomenon in metamorphic geology. In this review, it is defined as metamorphism on time scales that limit length scales (of the associated thermal anomaly) to significantly less than the thickness of the orogenic crust (<10 myr) or subducted oceanic lithosphere (<5 myr).” ↩
- 29a.
- 30.
Williams, Ian S. “Response of detrital zircon and monazite, and their U–Pb isotopic systems, to regional metamorphism and host-rock partial melting, Cooma Complex, southeastern Australia.” Australian Journal of Earth Sciences 48(4):557–580. 2001. A study of zircon and monazite grains in the Cooma Complex of southeastern Australia, a body of rock that was metamorphosed and partly melted to form granite. It follows how the grains changed from low to high grade metamorphism, and dates the metamorphism and granite formation to 433.4 ± 3.1 Ma, with cooling of about 12 °C per million years. The article uses it because Snelling relies on this paper for the Cooma cooling history, and its authors say that history fits the unroofing of a regional thermal high better than the cooling of an igneous intrusion.
- 30a.
Section Abstract: “Cooling of the metamorphic complex was relatively slow (average ∼12°C/10⁶y from ∼730 to ∼170°C), more consistent with the unroofing of a regional thermal high than cooling of an igneous intrusion.” ↩
- 30a.
- 31.
Thordarson, Thorvaldur, and Stephen Self. “The Roza Member, Columbia River Basalt Group: A gigantic pahoehoe lava flow field formed by endogenous processes?” Journal of Geophysical Research: Solid Earth 103(B11):27411–27445. Nov 10, 1998. A research paper in the Journal of Geophysical Research: Solid Earth on the Roza Member, a part of the Columbia River basalts that the title calls a gigantic lava flow field. Its pages run from 27,411 to 27,445 in the journal. The article uses it as the slowest published estimate of how long the Roza took to build, about 14 years, with its individual lobes taking months.
- 31a.
Section Abstract: Page 27,411. “The Roza Member represents a compound pahoehoe flood basalt lava flow field, with an area of ~40,300 km2 and a volume of ~1300 km3. … The results indicate that the emplacement of individual Roza lobes lasted for months to years and that the lava flow field was constructed over a period of at least 14 years.” ↩
- 31a.
- 32.
Sheldon, Nathan D. “Pedogenesis and geochemical alteration of the Picture Gorge subgroup, Columbia River basalt, Oregon.” Geological Society of America Bulletin 115(11):1377–1387. Nov 2003. A research paper in the Geological Society of America Bulletin on pedogenesis, meaning soil formation, and chemical alteration in the Picture Gorge subgroup of the Columbia River basalt in Oregon. The article uses it as the field test of whether the reddened layers between flows are fossil soils, which Woodmorappe and Oard deny.
- 32a.
Section Abstract: “Reddened, clay-rich horizons between basalt flows have historically been identified as 'baked zones' or as zones of lateral groundwater movement. The reddening has been attributed to thermal or chemical alteration of the permeable portion of the basalt flow. Many of these red horizons are instead paleosols that record significant hiatuses in basalt flow emplacement. Paleosols were identified in the field on the basis of features such as horizonation, ped morphology, and root traces. Terrestrial gastropods, fossil plants, and peats also occur locally.” ↩
- 32a.
- 33.
Höfig, Daianne et al. “Annually resolved sediments in the classic Clarkia lacustrine deposits (Idaho, USA) during the middle Miocene Climate Optimum.” Geology 49(8):916–920. Aug 2021. A 2021 research paper in Geology on the Clarkia lake deposits in Idaho, a lake dammed by a flood basalt flow. It dates the ash beds in the mud to 15.78 million years by U-Pb zircon dating, and it argues that about 7.5 m of laminated mud, called varves (yearly layers of sediment), represents about 840 years; it reads the abundant leaves in the fine autumn layers as a sign of seasonal deposition rather than storms. The article uses it as its counted lake, about 840 years in one gap between flows, more than twice the Flood year.
- 33a.
Section Abstract: “The flood basalt dammed a local drainage system to form the paleolake, which preserved a plant fossil Lagerstätte in its deposits. … We present the first unequivocal U-Pb zircon ages from interbedded volcanic ashes at the P-33 type location, constraining the deposition to 15.78 ± 0.039 Ma. … Consequently, the ~7.5-m-thick varved deposit at the type location P-33 represents ~840 yr of deposition, coincident with the end of the main phase of Columbia River Basalt Group eruptions during the Miocene Climate Optimum.” ↩ ↩
- 33a.
- 34.
Goehring, Lucas, and Stephen W. Morris. “Scaling of columnar joints in basalt.” Journal of Geophysical Research: Solid Earth 113:B10203. 2008. A 2008 physics paper on columnar joints, the cracks that split cooling basalt into columns. It finds that the column radius and the stria size are proportional to each other and inversely proportional to the cooling rate of the lava, and it reports Pe = 0.3 ± 0.1. The authors believe their conclusions apply to all igneous columnar joints. The article uses it as the measurement that column width tracks cooling rate.
- 34a.
Paragraph 1, section abstract: “We found that the column radius and stria size are proportional to each other and inversely proportional to the cooling rate of the lava.” ↩
- 34a.
- 35.
Závada, P. et al. “Devils Tower (Wyoming, USA): A lava coulée emplaced into a maar-diatreme volcano?” Geosphere 11(2):354–375. Apr 2015. A 2015 paper arguing that Devils Tower is the remnant of a lava coulée, a lava flow, not of an intrusion as most earlier studies held. Its three-dimensional thermal model of heat leaving the rock by conduction gives a total cooling time of about 4,000 years. The article uses that figure as the published cooling estimate it tests.
- 35a.
Section Devils Tower and Missouri Buttes Phonolite Bodies: Subsection Devils Tower, first paragraph. “The area above the base, which is also called the shoulder (Fig. 1D), consists of columns of the lower tier with diameters of 2–3 m. These columns taper to widths of only 1.5 m at the contact with the upper tier, where they frequently merge into one thick column (> 3 m wide) of the upper tier.” ↩
- 35b.
Section Discussion, thermal-modelling paragraph: “The 3-D thermal model that was constructed for the geometry of model D-19 also revealed that the total cooling time in the center of the hot core at the suture between the cooling fronts above the feeding conduit (Fig. SI-1 [see footnote 1]) corresponds to ∼4000 yr.” Model D-19 is the analogue coulée, “positioned at the base of the tower within a hypothetical 1-km-wide crater at the level of the Sundance Formation”. ↩
- 35a.
- 36.
Portenga, Eric W., and Paul R. Bierman. “Understanding Earth's eroding surface with ¹⁰Be.” GSA Today 21(8):4–10. Aug 2011. A compilation of 1,599 erosion rates measured with beryllium-10, a rare isotope that cosmic rays make in the top few metres of rock, so its amount shows how long the surface has been eroding. The two University of Vermont geologists gathered the rates from 87 studies around the world and standardized them so they could be compared. The article uses the median rate for bare rock outcrops, 5.4 m per million years, to test Oard's objection. The erosion-rates article discusses this compilation.
- 36a.
Page 4: From the abstract. “Drainage basins erode more quickly (mean = 218 m Myr⁻¹; median = 54 m Myr⁻¹) than outcrops (mean = 12 m Myr⁻¹; median = 5.4 m Myr⁻¹), likely reflecting the acceleration of rock weathering rates under soil.” Outcrops n = 450. ↩
- 36a.
- 37.
Meier, H., and W. Hecker. “Radioactive halos as possible indicators for geochemical processes in magmatites.” Geochemical Journal 10(4):185–195. 1976. A geochemistry paper by H. Meier and W. Hecker of the State Research Institute for Geochemistry in Bamberg, Federal Republic of Germany, which counted polonium halos in biotite mica from Norway and Ontario. It tested the halo centres for uranium by fission tracks, and ranked the halo types by abundance: ²¹⁰Po, then ²¹⁸Po, then ²¹⁴Po. The article cites it as independent confirmation that the halos exist; it is often miscited as a Nature paper, but it appeared in the Geochemical Journal.
- 37a.
Page 188: “it can be stated that no or only small amounts of uranium are present in polonium halos, a result, which agrees with the lack of uranium ring-structures in these halos.” The same page gives the sensitivity: “fission track studies allow a determination of uranium contents down to the ppm range.” ↩
- 37a.
- 38.
Gentry, Robert V. et al. “Radiohalos in Coalified Wood: New Evidence Relating to the Time of Uranium Introduction and Coalification.” Science 194(4262):315–318. Oct 15, 1976. A research report in Science by Robert Gentry and seven co-authors on radiohalos in coalified wood, which is wood that has turned to coal, from the Colorado Plateau. They measured halo ring radii and analysed the halo centres with x-ray and ion microprobes, and reported polonium-210 halos that formed from uranium daughter products carried into the wood by uranium-bearing solutions. The article uses it as Gentry's own evidence that polonium halos form by fluid transport.
- 38a.
Page 316: “Of the thousands of Po halos seen in this matrix, only three show any trace of a ring that could possibly be attributed to ²¹⁴Po α-decay [that is, from the accumulation of the U-daughters ²¹⁴Pb (t½ = 27 minutes), ²¹⁴Bi (t½ = 20 minutes), or ²¹⁴Po (t½ = 164 µsec)], and none has been seen with a ring from ²¹⁸Po α-decay [that is, from the accumulation of short-lived ²¹⁸Po (t½ = 3 minutes)].” ↩
- 38a.
- 39.
Wakefield, J. Richard. “Gentry's Tiny Mystery — Unsupported by Geology.” Creation/Evolution 8(1 (whole issue 22)):13–33. 1988. A popular article in the magazine Creation/Evolution, from its winter 1988 issue, on the geology of three of Gentry's sample sites near Bancroft, Ontario. It is the popular companion to Wakefield's refereed paper in the Journal of Geological Education. The article uses it to show that Gentry's sites are not primordial granite.
- 39a.
Page 30: “the samples of biotite that contain Gentry's polonium halos came from pegmatite dikes and calcite vein dikes which cross-cut metamorphosed volcanic, sedimentary, and igneous rock units. The dikes are clearly the last to have formed, not the first.” ↩
- 39a.
- 40.
Laney, R., and A. W. Laughlin. “Natural annealing of pleochroic haloes in biotite samples from deep drill holes, Fenton Hill, New Mexico.” Geophysical Research Letters 8(5):501–504. May 1981. Section Abstract: “Examination of 46 thin-sections of Precambrian metamorphic and igneous rocks from three deep drill holes in northern New Mexico reveals a narrow depth-temperature range for annealing of pleochroic haloes in biotite.” A 1981 study of biotite mica from deep drill holes in northern New Mexico, where the rock temperature is known at every depth. Heat erases radiohalos, a process called annealing, and the study found that it happens across a narrow range of temperatures. The full paper also has a depth-temperature table on p. 502, which the RATE authors cite. The article uses it as the source of the 150 °C figure on which the short time scale of the RATE model depends.
- 40a.
Section Abstract: “Annealing of the haloes is first observed in samples from a depth of 1850 m (134°C present temperature) and is complete in samples from a depth of 2120 m (151°C).” ↩
- 40a.
- 41.
Snelling, Andrew A. “Polonium Radiohalos: Still 'A Very Tiny Mystery'.” ICR Impact (333). Aug 1, 2000. A short article in Impact, an Institute for Creation Research publication, by Andrew A. Snelling. It predates the 2003 reversal. The article uses it for the 67,000-to-1 ratio, which it names as the sharpest unanswered problem in RATE's fluid-transport model, and for a concession about uranium.
- 41a.
“there should be 67,000 ²¹⁰Po radiohalos for each ²¹⁸Po radiohalo. Yet in a Norwegian biotite there are more than 1,000 ²¹⁰Po radiohalos, 90 ²¹⁸Po radiohalos and only one ²¹⁴Po radiohalo”. 138.4 days divided by 3.10 minutes is about 64,000, so the 67,000 implies a slightly shorter ²¹⁸Po half-life; the discrepancy does not affect the argument. ↩
- 41a.
- 43.
Ryan, Paul D., and John F. Dewey. “The sources of metamorphic heat during collisional orogeny: the Barrovian enigma.” Canadian Journal of Earth Sciences 56(5):525–545. 2019. A review article, not a set of new measurements, on where the heat for metamorphic rock comes from in mountain belts. It finds that conduction through a thickened crust cannot produce Barrovian rocks (medium temperature and medium pressure) in some short-lived mountain belts, such as Western Ireland and Timor. The article uses it for the conduction time formula, for its admission that conduction fails in short belts, and for its calculation of heating from radioactive rock.
- 43a.
Lines 314–319: “The known concentrations of K, U, Th for the Dalradian Supergroup in Ireland (O'Connor and Long 1985; Ahmed-Said and Leake 1990) would have raised temperatures by 17.5 - 30.0 °K.my⁻¹ (Figure 2B). Assuming that the sedimentary pile was initially at 150 °C temperatures would have only reached 290 – 390 °C after 8 my. The observed temperatures necessitated either heating rates of 50 – 75 °K.my⁻¹ (Figure 2B) or initial temperatures of approximately 400-500 °C before the onset of deformation. There is no evidence that either of these conditions existed.” ↩
- 43a.
- 44.
Humphreys, D. Russell. “Young Helium Diffusion Age of Zircons Supports Accelerated Nuclear Decay.” Radioisotopes and the Age of the Earth, Volume II, 25–100. Institute for Creation Research and Creation Research Society. Edited by L. Vardiman, A. A. Snelling and E. F. Chaffin. 2005. Chapter 2 of the 2005 young-earth creationist research volume, titled as an argument that the helium diffusion age of zircons is young. The helium argument itself is treated in the RATE and Helium in Zircons article. The article uses it for the temperature assumption in Humphreys' helium model.
- 44a.
Page 69: “Let us take as an example the x-value and temperature (197 °C = 470 K) of point 3 in Table 3, and a t of 6000 years. Then for a Δt of 1 year, T_h would be about 90 °C above today's temperature. For a Δt of 1 month, T_h would be about 140 °C hotter than today. If the heat pulse had been much hotter or longer than those typical values, the diffusion age we calculate would have been significantly less than 4000 years”. ↩
- 44a.
- 45.
House, Martha A. et al. “Paleo-geomorphology of the Sierra Nevada, California, from (U-Th)/He Ages in Apatite.” American Journal of Science 301(2):77–102. Feb 2001. A paper that dates Sierra Nevada granite by the helium trapped in apatite crystals, a mineral that records when a rock cooled through about 45 to 75 °C. It uses helium ages from 40 to 85 million years to reconstruct the landscape of the Late Cretaceous. The article uses it because this clock closes at low temperature, so it dates cooling near the surface rather than the crystallizing of the magma.
- 45a.
Page 82: Page 82 and abstract: “Helium ages from a new orogen-parallel, constant-elevation sample transect are relatively uniform (~60 Ma)”. “A large range of helium ages (40-85 Ma) from samples collected along a single structural datum”. ↩
- 45b.
Pages 81–82: “Presently exposed basement rocks are predominantly 125 to 80 Ma granite and granodiorite plutons of the Sierran magmatic arc”. “Thermobarometric data suggest crystallization pressures of most of these plutons (~80-100 Ma) at 100 to 300 MPa or about 4 to 12 km depth.” ↩
- 45a.
- 46.
Chenet, Anne-Lise et al. “Determination of rapid Deccan eruptions across the Cretaceous-Tertiary boundary using paleomagnetic secular variation: Results from a 1200-m-thick section in the Mahabaleshwar escarpment.” Journal of Geophysical Research: Solid Earth 113:B04101. Apr 30, 2008. A paper on the Deccan lava flows that reads the magnetic direction recorded in 1,200 m of flows at the Mahabaleshwar escarpment to work out how fast they erupted. Its abstract says the large eruptive events lasted a few decades each, with volumes of 3,000 to 20,000 km³. The Flood Basalts article uses it for the fastest Deccan figures and for the authors' remark that the eruptions were short compared with the gaps between flows.
- 46a.
Paragraph 56: “We finally estimate coarse bounds on the total amount of time recorded in the section by both volcanics and intertrappean levels to be between 85 + 2000 = 2085 yrs and 850 + 100,000 = 100,850 yrs. … Lack of correlation between successive magnetic directions implies that at least a few centuries (say >500 years) must have elapsed, adding yet another minimum of [(49 − 24) + 6 − 1] × 500 = 15,000 years to the total duration. The range of estimates then becomes 17,085 to 115,850 years, which we round up as 15 to 115 ka”. ↩
- 46a.
- 47.
Kasbohm, Jennifer, and Blair Schoene. “Rapid eruption of the Columbia River flood basalt and correlation with the mid-Miocene climate optimum.” Science Advances 4(9):eaat8223. Sep 19, 2018. A research paper in Science Advances on how fast the Columbia River basalts erupted, linked in its title to the mid-Miocene climate optimum, a warm spell in the middle Miocene. Its abstract says more than 95% of the Columbia River Basalt Group erupted between 16.7 and 15.9 million years ago, which the authors call twice as fast as earlier estimates. The Flood Basalts article uses it for the fastest published figure for the eruption.
- 47a.
Section Abstract, page 1: “Our data set shows that more than 95% of the CRBG erupted between 16.7 and 15.9 Ma, twice as fast as previous estimates.” ↩
- 47a.
- 48.
Li, Yongquan. “Columnar joints in intermediate and felsic volcanic rocks.” Research Square preprint rs-3031790/v1. Jul 7, 2023. A preprint, not peer reviewed, on columnar joints in intermediate and felsic volcanic rocks, the lavas that are rich in silica. It gives a simple formula for the cooling time, t = L²/α, where L is the side length of the column and α is the thermal diffusivity (how fast heat moves through the rock), and it works one example with a rhyolitic lava. The article uses it for that formula and not as an authority.
- 48a.
Page 9: “Therefore, cooling processes (slower or faster cooling rate) not affect the ordering behavior.” ↩
- 48a.
- 49.
Robinson, Charles S. “Geology of Devils Tower National Monument, Wyoming.” U.S. Geological Survey Bulletin 1021-I, 289–302. 1956. A survey of the Tower's geology, published by the US Geological Survey in 1956. It gives the Tower's height, base width, column sizes and rock type, and suggests the Tower is intrusive rock, rock that cooled underground from magma, that was never much larger than its present base. Robinson admits that no conclusive proof of how the Tower formed can be presented. The article uses it for the Tower's measurements, its massive base, and its claim that several hundred feet of rock covered the Tower when it formed.
- 49a.
Page 293: “At the base of the tower, below the bench, the rock is massive and jointing, poorly developed. Here the joints form large irregularly shaped blocks rather than columns.” ↩
- 49a.
- 50.
Henke, Kevin R. “Cooling Magmas: More Distortions from Snelling and Woodmorappe.” Greene's Creationism Truth Filter. Feb 13, 1999. A critique by Kevin R. Henke, Ph.D., originally posted to talk.origins on 13 February 1999, of Snelling and Woodmorappe's 1998 paper on how plutons (bodies of granite that cooled underground) cool. He says the paper leaves out the long cooling times in the sources it cites, and he concedes that some granite may be emplaced by dikes in a few thousand years. The article calls him their sharpest critic on this topic and uses his concession that fast emplacement is possible.
- 50a.
In the paragraph that opens with the words While geologists can accept rapid natural events: “Precambrian granites have much the same mineralogies, textures and structures as Cretaceous and other Phanerozoic granites, yet YEC dogma arbitrarily insists that Precambrian granites had a miraculous origin within a few days or less while Phanerozoic granites supposedly formed naturally over a maximum of a few thousand years.” ↩
- 50a.