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  • 1
    Monograph available for loan
    Monograph available for loan
    Washington, D.C. : Mineralogical Society of America
    Associated volumes
    Call number: M 92.0614 / Regal 11
    In: Reviews in mineralogy
    Description / Table of Contents: Unlike sedimentation and volcanism, active metamorphism is not directly observable. Metamorphic petrologists therefore must infer what constitutes the process of metamorphism by examining the products of metamorphic events. The purpose of this volume is to review the use of a powerful probe into metamorphic process: mineral assemblages and the composition of minerals. Put very simply, this volume attempts to answer the question: "What can we learn about metamorphism through the study of minerals in metamorphic rocks?" It is not an encyclopedic summary of metamorphic mineral assemblages; instead it attempts to present basic research strategies and examples of their application. Moreover, in order to limit and unify the subject matter, it concentrates on the chemical aspects of metamorphism and regrettably ignores other important kinds of studies of metamorphic rocks and minerals conducted by structural geologists, structural petrologists, and geophysicists. An overview of the chemical aspects of modern metamorphic petrology is timely because it brings together three areas of research which have reached maturity only in the last 25 years: (1) chemical analysis of minerals by microanalytical techniques; (2) application of reversible and irreversible thermodynamics to petrology; and (3) laboratory phase equilibrium experiments involving metamorphic minerals. Chemical thermodynamics is the formal mathematical framework which links measurable variables (i.e., mineral composition) to metamorphic variables which cannot be directly measured (i.e., chemical potential, pressure, temperature, fluid composition). Results of phase equilibrium studies involving metamorphic minerals at metamorphic pressures and temperatures (together with calorimetric and heat capacity data) permit these links to be quantitative. It is the union of analysis, theory, and laboratory experiment which allows the modern metamorphic petrologist to make sophisticated inferences about conditions of metamorphism and the factors which control these conditions. This union is the principal subject of the volume. The volume is organized much in the same way that one might approach a research project involving metamorphic rocks. Initially those chemical components which characterize the composition of minerals in the assemblages under consideration must be identified. In addition, the reaction relationships among components must be systematically characterized. The reaction relationships rationalize the prograde changes in mineralogy which rocks experience during metamorphism and, furthermore, form the basis for extracting information about intensive variables during metamorphism. Chapters 1-3 summarize strategies for identifying components in metamorphic minerals and for formulating chemical reactions among them. Chapter 4 develops, from classical thermodynamics, those equations which can be used to explicitly relate mineral composition to other variables of interest such as metamorphic pressure, temperature, and chemical potentials of volatile species in any metamorphic fluid phase. Chapter 5 is specifically devoted to geologic thermometry and barometry, and Chapter 6 reviews strategies for the determination of metamorphic fluid composition. Petrologists should not be content with simply calculating and cataloguing values of metamorphic pressure, temperature, and fluid composition. In order to characterize the process of metamorphism, we must try to understand what controls these measured values and the manner in which they evolve during metamorphism both as rocks are heated and buried and as rocks are cooled and uplifted. Chapter 7 explores how two concepts buffering and infiltration -- can act as general controls on fluid composition, mineral composition, and temperature during metamorphic events. In addition, this chapter develops procedures which can be used to evaluate the relative importance of buffering versus infiltration in the evolution of specific rocks. Chapter 8 demonstrates how integrated petrologic and stable isotope studies may be used, in principle, to reconstruct the prograde pressure-temperature-infiltration history of metamorphic rocks. Chapter 9 discusses the use of mineral inclusions and compositional zoning in minerals in evaluating both prograde and post-peak P-T paths of certain mineral assemblages. In addition, compositional zoning is considered as an indicator of cooling rates during post-peak uplift. Thus between Chapter I and Chapter 9 we go from the first step of describing a metamorphic mineral assemblage through a reconstruction of the physical state in which it crystallized to an analysis of what factors controlled that state and how it evolved with time. The contents of the volume reflect two themes which underlie modern research in metamorphic petrology. The first of these is an ever-increasing emphasis on the quantitative characterization of metamorphism. Current research less involves description and classification than calculation of intensive and extensive variables attained during metatamorphism. This volume hopefully serves as a text in the quantitative study of the chemical aspects of metamorphism. As a corollary to the emphasis placed on quantitative methods, we can see increasing attention paid to analytical as opposed to graphical treatments of mineral equilibria. Graphical representations, while undeniably valuable, can consider two (or at most three) independent variables. Analytical treatment of mineral equilibria is attractive because it rigorously keeps track of all variables pertinent to an equilibrium assemblage. The second theme is an increasing interest in the dynamics of metamorphism. Metamorphism obviously is not a static process -- it involves changes in pressure, temperature, mineral and fluid composition, etc. The classical static approach to quantitative metamorphic petrology, though, searches for the physical conditions of a unique pressure-temperature state which a rock or mineral assemblage records. Mineral equilibria are used to estimate single values of pressure, temperature, and fluid composition -- a sort of snapshot of what conditions were like. If mineral assemblages indeed represent a fossilized metamorphic state, then calculated P, T, Xi' however, simply represent a single point along the P-T-Xi-time path which a rock followed during metamorphism. Chapters 2, 7, 8, and 9 reflect an increasing interest among petrologists in the entire P-T-Xi-time path (or at least in more than one point along it). We can expect to see less satisfaction in the future with the snapshot model of metamorphism and more effort devoted to characterizing metamorphism as a dynamic process. Thus the volume not only summarizes time-honored current practices in quantitative metamorphic petrology, but hopefully also identifies some paths which may be followed in the future.
    Type of Medium: Monograph available for loan
    Pages: xiii, 397 S.
    Edition: 2nd printing
    ISBN: 0-939950-12-X , 978-0-939950-12-6
    ISSN: 1529-6466
    Series Statement: Reviews in mineralogy 10
    Classification:
    Petrology, Petrography
    Language: English
    Note: Chapter 1. Composition Space: An Algebraic and Geometric Approach by James B. Thompson, Jr., p.1 - 32 Chapter 2. Reaction Space: An Algebraic and Geometric Approach by James B. Thompson, Jr., p. 33 - 52 Chapter 3. Linear Algebraic Manipulation of N-Dimensional Composition Space by Frank S. Spear, Douglas Rumble III, anohn J.M. Ferry, p. 53 - 104 Chapter 4. Analytical Formulation of Phase Equilibria: The Gibbs' Method by Frank S. Spear, John M. Ferry, and Douglas D. Rumble III, p. 105 - 152 Chapter 5. Geologic Thermometry and Barometry by Eric J. Essene, p. 153 - 206 Chapter 6. Characterization of Metamorphic Fluid Composition Through Mineral Equilibria by John M. Ferry and Donald M. Burt, p. 207 - 262 Chapter 7. Buffering, Infiltration and the Control of Intensive Variables during Metamorphism by Jack M. Rice and John M. Ferry, p. 263 - 326 Chapter 8. Stable Isotope Fractionation During Metamorphic Devolatilization Reactions by Douglas0 Rumble, III, p. 327 - 354 Chapter 9. Compositional Zoning and Inclusions in Metamorphic Minerals by Robert J. Tracy, p. 355 - 397
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  • 2
    Electronic Resource
    Electronic Resource
    Palo Alto, Calif. : Annual Reviews
    Annual Review of Earth and Planetary Sciences 26 (1998), S. 255-287 
    ISSN: 0084-6597
    Source: Annual Reviews Electronic Back Volume Collection 1932-2001ff
    Topics: Geosciences , Physics
    Notes: Abstract Stable isotopic, mineralogical, and chemical alteration in metamorphic terranes is evidence for reactive fluid flow during metamorphism. In many cases, the amount and spatial distribution of the alteration can be quantitatively interpreted using transport theory in terms of fundamental properties of metamorphic flow systems such as time-integrated flux, flow direction, and Peclet number. Many estimates of time-integrated flux in the upper and middle crust are surprisingly large, 105-106 cm3 fluid/cm2 rock; estimates for the lower crust are much smaller. Rather than pervasive and uniform, reactive fluid flow in all metamorphic environments is channelized on scales of 〈1-104 m. Channelization results from heterogeneous permeability structures controlled by features such as lithologic layering, contacts, folds, fractures, and faults. Consequently flow may be in the direction of either decreasing or increasing temperature or isothermal. Site-specific thermal-hydrologic models of metamorphic terranes that explicitly consider chemical reactions and dynamic permeability structures will help resolve outstanding questions with regard to the driving forces and duration of flow, metamorphic permeability distributions, and how deformation controls fluid flow.
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    Contributions to mineralogy and petrology 91 (1985), S. 283-304 
    ISSN: 1432-0967
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences
    Notes: Abstract Hydrothermal alteration of Tertiary granites from Skye involed the reaction of igneous amphibole, biotite, ferroaugite, fayalite, alkali feldspar, plagioclase feldspar, magnetite, and ilmenite with aqueous fluid primarily to combinations of secondary alkali feldspar, chlorite and montmorillonite. Lesser amounts of muscovite, calcite, epidote, prehnite, zeolite, and pyrite also developed. During mineralogical alteration of the granites there was a net addition to rock of H and a net loss of Ca, Fe, and probably Na. There is no positive evidence for a significant change in their Al, Si, Mg, or K contents. Hydrothermal alteration of Skye granite involved not only large-scale migration of 18O, 16O, D, and H but also of Ca, Fe, and probably Na. Mineral thermometry combined with textural observations suggests that chemical, isotopic, and most mineralogical alteration were synchronous and occurred at 350°–450° C. Textural observations further suggest that the mechanism of isotopic exchange between granite and hydrothermal fluid primarily was solution/reprecipitation. Mineral thermometry and oxygen fugacity barometry indicate that some minerals in the granites — clear alkali and plagioclase feldspars, Fe-Ti oxides, biotite, fayalite, and probably amphibole and pyroxene — have compositions that record physical conditions during crystallization or at high temperatures slightly below the crystallization temperature (650°–750° C). These minerals have chemistries that were later unaffected by the hydrothermal event. Mineral thermometry also indicates that other minerals — turbid feldspar and all secondary minerals — have compositions that record physical conditions of hydrothermal alteration (350°–450° C). The isotope chemistries of the high-temperature minerals are inferred to be those in unaltered “normal” granite while the isotope chemistries of the low-temperature minerals are inferred to be those of minerals equilibrated with the hydrothermal fluid at low temperature. The close correspondence between the isotopic and major element composition of minerals in altered granites leads to an integrated mineralogic/isotopic model that considers the granites as composed of two families of minerals: an“igneous” family and a “hydrothermal” family. Comparison of data for altered Skye granites with data from hydrothermally altered synmetamorphic granites from Maine shows the important control that depth exerts on the isotopic composition and mineral chemistry of altered granites. Because the hydrothermal fluids that altered epizonal Skye granites were meteoric in origin, altered rocks are isotopically lighter than “normal” granite. In part because the hydrothermal fluids that altered the mesozonal granites from Maine were metamorphic in origin, altered rocks are isotopically heavier then “normal” granite. The hydrothermal event on Skye was shallow and hence short-lived; mineral-fluid reactions did not go to completion. Minerals in altered Skye granites therefore show large departures from both chemical and isotopic exchange equilibrium. The hydrothermal event in Maine was deeper and hence long-lived; reactions more closely approached equilibrium. Minerals in altered Maine granites therefore show a much closer approach to both chemical and isotope exchange equilibrium.
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  • 4
    Electronic Resource
    Electronic Resource
    Springer
    Contributions to mineralogy and petrology 95 (1987), S. 166-181 
    ISSN: 1432-0967
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences
    Notes: Abstract Alkali olivine basalts from Skye were simultaneously contact metamorphosed by Tertiary gabbro and granite intrusions and altered by the hydrothermal convection system that the plutons induced. Four metamorphic zones were mapped around the plutons. Furthest from the intrusions, in the primary olivine zone, metabasalts are composed of combinations of igneous olivine, augite, plagioclase, titaniferous magnetite, ilmenite, zeolites, gyrolite, sulfides, and chlorite-smectite intergrowths. Closer to the plutons, in the smectite zone, saponite and carbonate appear, primary olivine and gyrolite disappear, and zeolites decrease dramatically in abundance. Still closer to the plutons, in the amphibole zone, actinolite, edenite, chlorite, sphene, epidote, andradite, and quartz appear and saponite and chlorite-smectite intergrowths disappear. Along parts of the contact between gabbro and basalt, in the orthopyroxeneolivine zone, orthopyroxene, metamorphic olivine, and biotite appear and amphibole, chlorite, sphene, epidote, andradite, carbonate, and quartz disappear. Whole-rock chemical data indicate only minor change in the major-element chemical composition of the metabasalts during progressive metamorphism/hydrothermal alteration. Two-pyroxene eothermometry and various mineral-fluid equilibria suggest the range of peak temperatures attained in the metamorphic zones: orthopyroxene-olivine zone, ∼900°1, 030° C; amphibole zone, ∼400°–900° C; smectite and primary olivine zones, 〈 400° C. Mineralogical and oxygen isotopic alteration of the metabasalts were closely coupled: Basalts from the primary olivine zone with nearly unaltered igneous mineralogies have normal or near-normal wholerock δ 18O〉+5‰ (SMOW); mineralogically more altered basalts from the smectite zone have whole-rock δ 18O=+2 to +5‰; still more mineralogically altered basalts from the amphibole zone (with one exception) have δ 18O〈+ 2‰; completely recrystallized hornfelses from the orthopyroxene-olivine zone have δ 18O〈0‰. The principal mechanism of isotope exchange between basalt and metamorphic/ hydrothermal fluid probably was heterogeneous mineralfluid reaction. Metabasalts from the orthopyroxene-olivine zone are mineralogically fresh pyroxene hornfelses that record crystallization temperatures 〉 1,000° C yet have highly altered whole-rock oxygen isotope compositions, δ 18O〈0%. The hornfelses chemically interacted with metamorphic/hydrothermal fluids either at very high temperatures or while they were heated to 〉 1,000° C or both. Their mineralogy, however, rules out significant water-rock interaction after they cooled below ∼900° C. Hydrothermal convection on Skye was a two-stage process: (a) fluid flow through wall rocks initially was pervasive while they are heated; (b) fluid flow after the thermal peak in the wall rocks was sufficiently channelized that rocks such as those in the orthopyroxeneolivine zone were isolated from further fluid-rock interaction during all or almost all of the cooling history of the hydrothermal system.
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  • 5
    Electronic Resource
    Electronic Resource
    Springer
    Contributions to mineralogy and petrology 91 (1985), S. 264-282 
    ISSN: 1432-0967
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences
    Notes: Abstract Hydrothermal alteration of Tertiary gabbros from Skye involved the reaction of igneous olivine, augite, hypersthene, plagioclase, magnetite, and ilmenite with aqueous fluid primarily to combinations of talc, chlorite, montmorillonite, calcic amphibole, biotite, and secondary magnetite. Lesser amounts of calcite, epidote, quartz, sphene, prehnite, and garnet also developed. During mineralogical alteration of gabbro there was a net addition to rock of K, Na, Sr, and H2O and a net loss of Mg. Gabbro was oxidized early in the hydrothermal event and later reduced. Iron and silicon were probably initially lost and later added. There is no evidence for significant change in the Al or Ca content of the gabbros. Hydrothermal alteration of Skye gabbro involved not only large-scale migration of 18O, 16O, D and H but also of K, Na, Sr, Mg, and probably Fe and Si. Mineral thermometry indicates that pyroxenes in the gabbros crystallized at 1000° C–1150° C and were very resistent chemically as well as isotopically to later hydrothermal alteration. Hypothetical equilibrium between primary and secondary mafic silicates suggests that mineralogical alteration of gabbro occurred at ∼450°–550° C. The lack of correlation between mineralogical and isotopic alteration of gabbro requires that much isotopic alteration occurred at temepratures above those at which the secondary minerals developed, 550°–1000° C. The chemical alteration of gabbro is correlated with its mineralogical alteration and therefore occurred at 450°–550° C. Measured progress of the mineral-fluid reactions was used to estimate the amount of H2O fluid that infiltrated the gabbro as primary olivine was converted to talc+magnetite at 525°–550° C. Calculated fluid-rock ratios are in the range 0.2–6 (volume basis) and are smaller than values estimated from isotopic data (fluid/rock ∼1–10, volume basis). Both isotopic and petrologic data point to pervasive flow of fluid through crystalline rock at elevated temperatures of 500°–1000° C. Isotopic fluid-rock ratios are larger than petrologic fluid-rock ratios because isotopic alteration of cooling gabbro began earlier and at higher temperatures than did the mineralogical alteration.
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  • 6
    Electronic Resource
    Electronic Resource
    Springer
    Contributions to mineralogy and petrology 87 (1984), S. 138-148 
    ISSN: 1432-0967
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences
    Notes: Abstract Taking account of the C¯1/I¯1 (Al/Si order/disorder) transformation at high temperatures in the albite-anorthite solid solution leads to a simple model for the mixing properties of the high structural state plagioclase feldspars. The disordered (C¯1) solid solution can be treated as ideal (constant activity coefficient) and, for anorthite-rich compositions, deviations from ideality can be ascribed to cation ordering. Values of the activity coefficient for anorthite in the C¯1 solid solution (γ An C¯1 ) are then controlled by the free energy difference between C¯1 and I¯1 anorthite at the temperature (T) of interest according to the relation: Δ¯G ord I¯1 ⇌C¯1 =RT ln γ An C¯1 . If the I¯1⇌C¯1 transformation in pure anorthite is treated, to a first approximation, as first order and the enthalpy and entropy of ordering are taken as 3.7±0.6 kcal/mole (extrapolated from calorimetric data) and 1.4–2.2 cal/mole (using an equilibrium order/disorder temperature for An100 of 2,000–2,250 K), a crude estimate of γ An C¯1 for all temperatures can be made. The activity coefficient of albite in the C¯1 solid solution (γ Ab C¯1 ) can be taken as 1.0. The possible importance of this model lies in its identification of the principal constraints on the mixing properties rather than in the actual values of γ An C¯1 and γ Ab C¯1 obtained. In particular it is recognised that γ An C¯1 depends critically on ordering in anorthite as well as, at lower temperatures, any ordering in the C¯1 solid solution. A brief review of activity-composition data, from published experiments involving ranges of plagioclase compositions and from the combined heats of mixing plus Al-avoidance entropy model (Newton et al. 1980), reveals some inconsistencies. The values of γ An C¯1 calculated using the approach of Newton et al. (1980), although consistent with Orville's (1972) ion exchange data, are slightly lower than values derived from experiments by Windom and Boettcher (1976) and Goldsmith (1982) or from ion-exchange experiments of Kotel'nikov et al. (1981). Based on the C¯1/I¯1 transformation model, values of γ An C¯1 〈1.0 are unlikely. Discrepancies between the experimental data sets are attributed to incomplete (non-equilibrium) Al/Si order attained during the experiments. It is suggested that the choice of activity coefficients remains somewhat subjective. The development of accurate mixing models would be greatly assisted by better thermodynamic data for ordering in pure anorthite and by more thorough characterisation of the state of order in plagioclase crystals used for phase equilibrium experiments.
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  • 7
    Electronic Resource
    Electronic Resource
    Springer
    Contributions to mineralogy and petrology 93 (1986), S. 420-428 
    ISSN: 1432-0967
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences
    Notes: Abstract Hydrothermally-altered mesozonal synmetamorphic granitic rocks from Maine have whole-rock δ 18O (SMOW) values 10.7 to 13.8‰. Constituent quartz, feldspar, and muscovite have δ 18O in the range 12.4 to 15.2‰, 10.0 to 13.2‰, and 11.1 to 12.0‰, respectively. Mean values of Δ Q−F (δ 18Oquartz−δ 18Ofeldspar)=2.4 and Δ Q−M (δ 18Oquartz−δ 18Omuscovite)=3.3 are remarkably uniform (standard deviations of both are 0.2). Measured Δ Q−F and Δ Q−M values demonstrate that the isotopic compositions of the minerals are altered from primary magmatic δ 18O values but that the minerals closely approached oxygen isotope exchange equilibrium at subsolidus temperatures. Analyzed muscovites have δD (SMOW) values in the range −65 to −82‰. Feldspars in the granitic rocks are mineralogically altered to either (a) muscovite+calcite, (b) muscovite+calcite+epidote, (c) muscovite+epidote, or (d) muscovite only. A consistent relation exists between the assemblage of secondary minerals and the oxygen isotope composition of whole rocks, quartz, and feldspar. Rocks with assemblage (a) have whole-rock δ 18O〉12.1‰ and contain quartz and feldspar with δ 18O〉13.8‰ and 〉11.4‰, respectively. Rocks with assemblages (b), (c), and (d) have whole-rock δ 18O〈11.4‰ and contain quartz and feldspar with δ 18O〈 13.1‰ and 〈11.0‰, respectively. The correlation suggests that the mineralogical alteration of the rocks was closely coupled to their isotopic alteration. Three mineral thermometers in altered granite suggest that the hydrothermal event occurred in the temperature range 400°–150° C, ∼100°–150° C below the peak metamorphic temperature inferred for country rocks immediately adjacent to the plutons. Calculations of mineral-fluid equilibria indicate that samples with assemblage (a) coexisted during the event with CO2-H2O fluids of $${\text{X}}_{{\text{CO}}_{\text{2}} } = 0.03 - 0.13$$ and δ 18O=10.8 to 12.2‰ while samples with assemblages (b), (c), or (d) coexisted with fluids of $${\text{X}}_{{\text{CO}}_{\text{2}} } \leqslant 0.03$$ and δ 18O=9.4 to 10.1‰. Compositional variations of the hydrothermal fluids were highly correlated: fluids enriched in CO2 were also enriched in 18O. Because CO2 was added to the granites during hydrothermal alteration and because fluids enriched in CO2 were enriched in δ 18O, some or all of the variation in δ 18O of altered granites may have been caused by addition of 18O to the rocks during the hydrothermal event. The source of both the CO2 and 18O could have been high-18O metasedimentary country rocks. The inferred change in isotopic composition of the granites is consistent with depletion of the metacarbonate rocks in 18O close to the plutons and with large volumes of fluid that were inferred from petrologic data to have infiltrated the metacarbonate rocks during metamorphism. A close approach of minerals to oxygen isotope exchange equilibrium in altered mesozonal rocks from Maine is in marked contrast to hydrothermally-altered epizonal granites whose mineral commonly show large departures from oxygen isotope exchange equilibrium. The difference in oxygen isotope systematics between altered epizonal granites and altered mesozonal granites closely parallels a differences between their mineralogical systematics. Both differences demonstrate the important control that depth exerts on the products of hydrothermal alteration. Deeper hydrothermal events occur at higher temperature and are longer-lived. Minerals and fluid have sufficient time to closely approach both isotope exchange and heterogeneous chemical equilibrium. Shallower hydrothermal events occur at lower temperatures and are shorter-lived. Generally there is insufficient time for fluid to closely approach equilibrium with all minerals.
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  • 8
    Electronic Resource
    Electronic Resource
    Springer
    Contributions to mineralogy and petrology 99 (1988), S. 401-415 
    ISSN: 1432-0967
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences
    Notes: Abstract Crystal size distributions (CSDs) measured in metamorphic rocks yield quantitative information about crystal nucleation and growth rates, growth times, and the degree of overstepping (ΔT) of reactions during metamorphism. CSDs are described through use of a population density function n=dN/dL, where N is the cumulative number of crystals per unit volume and L is a linear crystal size. Plots of ln (n) vs. L for olivine+pyroxene and magnetite in high-temperature (1000° C) basalt hornfelses from the Isle of Skye define linear arrays, indicating continuous nucleation and growth of crystals during metamorphism. Using the slope and intercept of these linear plots in conjunction with growth rate estimates we infer minimum mineral growth times of less than 100 years at ΔT〈10° C, and nucleation rates between 10−4 and 10−1/cm3/s. Garnet and magnetite in regionally metamorphosed pelitic schists from south-central Maine have CSDs which are bell-shaped. We interpret this form to be the result of two processes: 1) initial continuous nucleation and growth of crystals, and 2) later loss of small crystals due to annealing. The large crystals in regional metamorphic rocks retain the original size frequency distribution and may be used to obtain quantitative information on the original conditions of crystal nucleation and growth. The extent of annealing increases with increasing metamorphic grade and could be used to estimate the duration of annealing conditions if the value of a rate constant were known. Finally, the different forms of crystal size distributions directly reflect differences in the thermal histories of regional vs. contact metamorphosed rocks: because contact metamorphism involves high temperatures for short durations, resulting CSDs are linear and unaffected by annealing, similar to those produced by crystallization from a melt; because regional metamorphism involves prolonged cooling from high temperatures, primary linear CSDs are later modified by annealing to bell shapes.
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  • 9
    Electronic Resource
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    Springer
    Contributions to mineralogy and petrology 98 (1988), S. 1-12 
    ISSN: 1432-0967
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences
    Notes: Abstract The flow pattern of reactive metamorphic fluid through six outcrops of micaceous, carbonate-bearing sandstones from the Vassalboro Formation was determined by calculating and mapping fluid-rock ratios for numerous samples within each outcrop. The ratio of maximum to minimum measured fluid/rock varied by factors of only 1.3-22.9 in each outcrop. Fluid flow was pervasive at metamorphic grades ranging from the biotite through the sillimanite zones. Average fluid-rock ratio for the outcrops increases with increasing grade of metamorphism from ∼0.4 in the biotite zone to ∼ 1.4 in the sillimanite zone. The flow pattern of reactive fluid through impure sandstones of the Vassalboro Formation was different at low and medium grades from fluid flow through the limestone member of the adjacent Waterville Formation. In the biotite and garnet zones, fluid flow through the Waterville Formation was channelized with channelways corresponding to individual lithologic layers that acted as metamorphic aquifers. Fluid-rock ratios recorded by the aquifers are greater than those recorded by the intervening beds by factors of up to 50–60. At the highest grades of metamorphism (sillimanite zone), however, flow through the Waterville Formation was as pervasive as through the Vassalboro Formation. The Waterville and Vassalboro Formations experienced the same metamorphic event. The difference in pattern of fluid flow through the two formations therefore reflects the important control that lithology exerts on the permeability of rocks during metamorphism. Micaceous, carbonate-bearing sandstones evidently were more permeable than argillaceous carbonate rocks. The greater permeability of the sandstones may result from a greater concentration of grain boundaries between unlike minerals in the rocks.
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  • 10
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    Springer
    Contributions to mineralogy and petrology 101 (1989), S. 402-417 
    ISSN: 1432-0967
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences
    Notes: Abstract Calcareous hornfelses and marbles all contain calcite+K-feldspar+quartz+sphene±diopside±plagioclase ±scapolite±clinozoisite. In addition, rocks on one side of a fault contain combinations of biotite, amphibole, and muscovite while those on the other side contain combinations of grossular, wollastonite, and axinite. At $$P = p_{{\text{CO}}_{\text{2}} } + P_{{\text{H}}_{\text{2}} {\text{O}}} = 2000$$ bars, mineral-fluid equilibria in biotite and amphibole-bearing rocks record T=∼ 440° C and $$X_{CO_2 } = 0.04 - 0.05$$ garnet-bearing rocks record T=∼540° C and $$X_{CO_2 } = 0.04 - 0.05$$ Conventional volumetric fluid-rock ratios were calculated using measured progress of prograde decarbonation reactions and the $$P - T - X_{CO_2 } $$ conditions of metamorphism: marbles, 0–0.4; amphibole-bearing hornfelses, 1.0–1.4; garnet-bearing hornfelses, 2.8–6.7. Decarbonation reactions were driven by pervasive infiltration of rock by reactive aqueous fluids. Differences in fluid-rock ratio between interbedded marble and hornfels and lack of correlation between fluid-rock ratio and whole-rock Cl-content, however, argue for channelized fluid flow along lithologic layers. A new analysis of reaction progress allows estimation of time-integrated fluxes for a specified temperature gradient along the direction of flow. Results are: marbles, 0–0.1×105 cm3/cm2; amphibole-bearing hornfelses, 0.8–1.3×105 cm3/cm2; garnet-bearing hornfelses, 1.2–2.5 × 105 cm3/cm2. Fluid flowed from regions of low to regions of high temperature. Using a simple thermal model for the area, the duration of contact metamorphism was estimated as 105 years. Assuming the time of fluid flow was the same as the duration of the thermal event, the first “measurements” of average metamorphic fluxes (q) and permeabilities (k) are: average marbles, q=0–0.3×10−8 cm/s and k =≤2×10−6 darcy; hornfels, q=3–8×10−8 cm/s and k =20–53×10−6 darcy. Estimated premeabilities are within the range of values measured for metamorphic rocks in the laboratory. Fluxes, permeabilities, and whole-system fluidrock ratios are similar to those estimated for the Skaergaard hydrothermal system by Norton and Taylor (1979).
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