5.1. Combustion Metamorphism: Processes and Products
Combustion metamorphism is a type of thermal metamorphism involving very high temperatures often to the point of causing melting at very low (often ambient) pressure. Nominally CM rocks were classified by Callegari and Pertsev [
40] and by Grapes [
11] as sanidinite facies contact metamorphics but making a particular genetic group due to an unusual heat source. Combustion metamorphic or pyrometamorphic (annealed, melted, and slag-like) rocks are produced by in situ natural combustion of fossil fuels and are typical geological features in many coal deposits, some oil basins, and regions of bituminous sedimentation. High-temperature (up to 1000 °C) and especially ultrahigh-temperature (1200–1500 °C), low pressure thermal effects are usually restricted to very narrow spots heated and/or melted by burning gas [
7,
14,
25,
53]. Such CM varieties, and even enormous amounts of molten and quenched rocks, formed sometimes in the Late Cenozoic in zones where bitumen in sediments and gas were burning together or where burning occurred within gas traps [
4,
53,
54,
55].
Fossil fuel combustion as a specific heat source that causes CM alteration of sediments has several features: (1) an abrupt temperature rise to 1000–1500 °C in the flame zone; (2) convective heat and mass transfer; (3) pyrolysis and in situ gasification of solid fuel in the zone of restricted oxygen flow. Such heat sources create extremely high temperature gradients with variations of hundreds °C over a few meters or even centimeters [
5,
7,
11,
14,
16,
17,
25]. The thermal impact of short to extremely short duration creates a unique mineral-forming environment: rapid decomposition of precursor sedimentary minerals, delamination and dihydroxylation of phyllosilicates, degassing, metastable melting, and growth of high-temperature minerals driven by significant temperature overstepping of equilibrium conditions. Although being of far more limited occurrence than other metamorphic facies, CM rocks are remarkable in a particular phase composition with crystalline and amorphous phases. The latter include thermally decomposed precursor phases in lower temperature assemblages and glasses in higher-temperature ones. The particular compositions (assemblages of minerals, glasses, and amorphous phases), textures, and crystal habits result from the effects of high temperature and chemical disequilibrium caused by incomplete reaction due to rapid heating and quenching. Generally, the distribution patterns of phases, as well as the specific morphology of quench solids (skeletal or hopper-like crystals, clasts of laths in glass), and the alignment of crystals around vesicles are common to paralava, iron sinter, and smelter slag, which indicates rapid crystallization from a melt [
6,
10,
11].
Ultrahigh-temperature CM alteration is marked by (i) the presence of glass in pelitic lithologies; (ii) unusual melt compositions produced by bulk melting of dehydrated and decarbonated sediments along with melts compositionally similar to anhydrous silicate eutectic melts; and (iii) crystallization of minerals from anhydrous melts and their quenching morphology. The paralavas are generally characterized by large variety of textures and non-hydroxyl-bearing high-temperature minerals, including quench crystals of tridymite, low-silica plagioclase, potassium feldspar, fayalite, ortho- and clinopyroxenes, wollastonite, mullite, gehlenite-rich melilite solid solutions, Fe-bearing cordierite, and Fe- and Al-rich spinel. The paralava glass formed by very rapid quenching looks felt-like or becomes a structureless matrix impregnated with abundant tiny grains of anhydrous silicates and opaque minerals [
4,
6,
10,
11,
15,
20,
41].
At moderate temperatures (T < 900 °C) or at a brief contact with rapidly dissipated hot gas, the metasedimentary substrate does not melt, but primary H
2O- or (OH)-bearing minerals become dehydrated and dehydroxylated, whereby the precursor phyllosilicates decompose to a mixture of amorphous compounds. The processes of long-range disordering coupled with water loss are known as amorphization [
11]. The CM alteration occurring at T < 900 °C also includes (i) decomposition of carbonate minerals; (ii) generation of intergranular melt films in pelitic lithologies; (iii) peripheral fusion of grains, and related induration of the heated rocks; and (iv) oxidation of iron and related reddening of iron-enriched (siderite- or pyrite-bearing) rocks [
11,
20,
41]. These rocks preserve only detrital quartz intact and resemble bricks in appearance, mode of formation, and strength, and are commonly classified as red clinker.
To sum up, the strong overheating (especially from burning gas), high viscosity of dry Ca-depleted, Al-rich silicate melts, and extremely rapid quenching of heated or melted compounds after the instantaneous flare extinguishing leaves no chance for the CM rocks to develop equilibrium assemblages [
11]. This is a prominent feature of ultrahigh-temperature Al- and Si-rich CM rocks produced by gas fires. Therefore, such systems often step over the mineral equilibrium lines and the related assemblages lack many phases that would appear in slower (quasi-equilibrium) processes. The probability of phase transitions and the sequence of crystallization are controlled in this case by the kinetics of the process (Ostwald step rule) rather than by thermodynamics [
11].
5.2. Regime of Combustion Metamorphism Caused by MV Fire Eruptions
The obtained data from the Karabetova Gora MV site have petrogenetic implications for mud exposed to the thermal impact of a gas flare. Bulk melting of the dehydrated pelitic protolith was limited to a 3–5 mm rim near the surface of blocks or locally produced flow structures, while spot melting was traceable until 1.5 cm below the surface. In addition to anhydrous Al-silicate glass, we identified in the Karabetova Gora CM rocks high-temperature, low-pressure index minerals, such as tridymite, cristobalite, and mullite in melt rocks, which taken together, they reveal the sanidinite facies conditions of metamorphism. The mineralogical conclusions are supported by the SigmaFlow numerical simulation of temperature (1400–1540 °C) for the flare core (
Figure 8) and the known ambient pressure.
The impact of the ultrahigh-temperature heat pulse already decayed rapidly 2 cm below the surface of the annealed blocks where mud breccia remained unmolten and preserved its original texture. Judging by the preservation of quartz and feldspar, the temperature was no higher than 870 °C. The principal high-temperature processes in the 2 cm outer zone below the molten crust included solid-phase clinkering and recrystallization of dehydrated and dehydroxylated amorphous Al-silicate matter. The heat pulse produced a high temperature gradient (at least 250 °C/cm) within 2 cm below the surface in the target material, which apparently changed in a nonlinear way and was the greatest near the surface. High redox gradients were additionally inferred from the presence of ferrous spinel coexisting with ferrous pyroxene and cordierite in the molten outer zone, as well as the preservation of authigenic pyrite at a depth of 2.5 cm.
The CM products of the Karabetova Gora MV eruption are remarkable by prominent heterogeneity even within 0.3 mm × 0.3 mm molten spots: different phase compositions in neighboring spots and diversity of newly formed silicates and glasses. The fast cooling of vitreous samples was confirmed further by typical quench morphology of newly formed phases, as well as by mosaic distribution of high-temperature mineral assemblages (
Figure 5,
Figure 6 and
Figure 7). The thermally altered rock is actually a snapshot of micro-variations in the protolith composition. Anhydrous and Ca-poor silicate CM melts failed to become compositionally homogeneous due to their high viscosity (10
2.0–10
2.3 Pa·s; T = 1400 °C; calculated using the method of Persikov and Bukhtiyarov [
56]) and the brevity of exposure to ultrahigh temperatures. Furthermore, both factors impeded crystallization of solids and glass devitrification. Indeed, the total amount of newly formed high-temperature crystalline phases in the Karabetova Gora paralavas was as low as 10–21 wt% (
Table 2).
The timescale of the exposure to burning gas is impossible to estimate exactly, but possible bounds are justifiable. The rocks were exposed to the gas flare for a few seconds (a few tens of seconds at most), from the firing time (explosion) until the time when the block fell on the ground. The heat dissipation timescales for the molten outer zone and the thermally affected interior were apparently different: the former was likely air quenched mode [
57,
58], whereas the block interior under the insulating quenched coat was cooling down for a few hours. Heating at such high rates (≥100 K/s) is classified as a thermal shock in the respective technological protocols. Thus, the outer zone of the blocks actually underwent a thermal shock, with instantaneous inhomogeneous heating, which produced high temperature gradients.
The phase and textural heterogeneity of the Karabetova Gora CM rocks provide strong evidence of local disequilibria in the system. The SigmaFlow numerical simulation yielded an estimate of 1400–1540 °C for the flare core (
Figure 8), while the 1500–1800 °C maximum temperature of methane burning in air [
59] can be considered as the upper temperature limit. The target material surface reached these temperatures for a few seconds at the longest. Therefore, any direct analogy with experimentally investigated petrological and technological (mainly ceramic) systems requires much caution in this case.
5.3. Was the Karabetova Gora MV Gas Flare a Highly Energetic Fast Geological Event?
Melting triggered by CM ultrahigh-temperature events is a non-equilibrium process which differs substantially from equilibrium magma generation. All magmatic melts are formed slowly at relatively low temperatures and correspond to eutectic compositions, whereas the natural CM events triggered by gas fires are extremely brief, and their culmination (up to 1500 °C) lasts at least a few seconds [
16,
17]. Unlike the slow magma generation, the rapid temperature rise at fire foci leads to the formation of non-eutectic melts compositionally similar to the bulk devolatilized sedimentary protolith [
4,
11,
15,
20]. In this respect, the Karabetova melt rocks are typical ultrahigh-temperature CM varieties. Non-equilibrium bulk melting of target materials on the ground surface can result from yet another brief ultrahigh-temperature, low-pressure natural event: lightning-induced terrestrial pyrometamorphism, which produces fulgurites [
41]. It is a highly energetic, fast geological event, in which a huge amount of energy is supplied to the target systems in fractions of a second and the heating rates reach ≥100 K/s [
60,
61,
62] at microsecond timescales [
63]. Such an amount of heat is able to melt/vaporize inorganic materials and to cause volatilization of most of major elements and formation of melts enriched in silica and depleted in alkalis [
41]. Extremely fast cooling of such melts produces homogeneous high-silica glass [
60]. Fulgurites commonly enclose micrometer-size globules of reduced compounds of metals (Fe, Si), silicides (FeSi, Fe
3Si
7, FeTiSi
2), and phosphides (TiP, Fe
3P) coexisting with vesicular silica-rich (82–99 wt% SiO
2) glass, residual undermolten quartz, and graphite [
11,
63]. However, the Karabetova CM rocks differ from fulgurites as the protolith only lost Na and Si, the redox conditions in the mineral-forming medium were oxidative, and Fe
2+- and Fe
3+-bearing oxygenated compounds were formed instead of native elements, phosphides, or silicides. The highest-temperature stage of the Karabetova CM event triggered by gas combustion was six orders of magnitude longer than lightning-induced melting. Thus, the obvious difference of Karabetova paralavas from fulgurites does not allow interpreting the gas fire-related pyrometamorphism as a highly energetic fast geological event.
The compared mineral-forming systems contain specific sets of chemical compounds. Annealed and fused metapelitic CM rocks tend to lose more than 90% of volatiles and up to 2/3 Na, but not potassium. As a result, CM melts are K-Al silica-rich and crystallize to form anhydrous Na-depleted mineral assemblages, mostly simple anhydrous oxides and silicates of major elements (Si, Al, Fe, Mg, Ca, Ti, K). In the known ordinary cases of natural and human-induced coal fires, CM assemblages are formed in the conditions of (i) high temperature, low pressure, and heating duration from several months to several years in any local spot; (ii) high chemical heterogeneity of sedimentary protoliths; (iii) gas convection; and (iv) high temperature and redox gradients. Jointly, these conditions lead to the formation of exceptionally diverse prograde CM mineral assemblages. They are especially diverse in hybrid rocks resulting from high-temperature alteration of carbonate and pelitic substrates, marly and phosphatic sediments with high trace-element loading, as well as molten rocks and assemblages of gas transport in gas chimneys. In these cases, a lot of minor and trace elements (F, Cl, P, S, Se, As, Sr, Ba, Zn, Cd, Cr, Ni, Mn, Mo, U, Pb, Ce, Th, Zr, Sn) become important mineral-forming agents besides the major elements (O, Si, Al, Fe, Mg, Ca, Ti, K, and rarer Na), and yield numerous combinations from bi-element to six-element compounds [
13,
15,
20,
26,
50,
55,
64,
65,
66,
67].
Contrary to these highly productive systems, the mineralogical productivity of the Karabetova Gora metapelitic CM rocks (
Figure 9) was as low as 1.38 (K = M
minerals/N
elements = 11/8), and is one of lowest among all CM rock samples in this study and in published evidence [
13,
14,
16,
17,
55]. The low mineralogical diversity is due to narrow ranges of formation conditions and protolith compositions (monotonic shales), as well as to polymerization of dry high-silica melts during quenching. The mineralogy of the Karabetova Gora CM rocks includes only oxygenated compounds, mostly bi- or three-element: three species of oxides (Si-O and Fe-O), three species of double oxides (Fe-Ti-O and Mg-Fe-O), and one simple Al silicate (Al-Si-O). Four mineral species consist of five elements, all silicates: pigeonite (Ca-Mg-Fe-Si-O), cordierite (Mg-Fe-Al-Si-O), labradorite, and bytownite (Ca-Na-Al-Si-O).
Importantly, CM alteration of low-Ca clayey protoliths in the three compositionally similar mineral-forming systems differs markedly in the duration of the high-temperature stage, as well as in the rates of melt cooling and quenching (
Figure 9). As the duration of the thermal impact increases from seconds (Karabetova Gora MV) to hours (Shikhzairli MV) and on to days/months (Kuznetsk coal basin), crystalline phases in CM rocks form in progressively higher percentages, while the amount of glass decreases from 70–80 wt% to 10–30 wt%. The mineralogical productivity is the highest (K = 1.8) in CM rocks formed in coal fires (Kuznetsk Coal Basin) but is low (K~1.3) in those from both Karabetova Gora and Shikhzairli MVs produced by brief events. The inverse correlation of mineralogical productivity in CM rocks with duration of high-temperature events indicates that it is kinetically controlled in fast ultrahigh-temperature events. In this respect, mineralogical productivity can be a proxy of CM event duration for compositionally similar CM rocks.
Thus, the natural thermal events such as onshore MV fire eruptions and their products have their specificity. Although being extremely short (second-to-minute timescales) and high-temperature (up to 1500 °C), they are yet inferior to highly energetic fast geological events that last a few milliseconds and reach a temperature of 2000 K [
11,
41]. Meanwhile, catastrophic offshore MV fire eruptions are still shorter than other ultrahigh-temperature natural CM events. Some events of this kind leave a “foam” consisting of hollow glass microspheres, like those floating on the surface of the Caspian Sea, known under the name “lapilli” [
68]. They arise by the same mechanism as microspheres in fly ash at thermal power plants [
69,
70]: bulk melting of dispersed mud drops in giant (400–500 m height) gas flares that are quenched in sea water. This extreme CM process may be the closest to highly energetic fast geological events.