GEOCHEMISTRY AND REACTION PATH MODELING OF THE BEOWAWE
HYDROTHERMAL SYSTEM, NEVADA: A BARREN END-MEMBER
EPITHERMAL SYSTEM
______
A Thesis Presented to
the Faculty of the Graduate School
University of Missouri-Columbia
______
In Partial Fulfillment
of the Requirements for the Degree
Master of Science
______
by
Mark Leatherman
Dr. Martin Appold, Thesis Supervisor
December 2010
The undersigned, appointed by the Dean of the Graduate School, have examined the thesis entitled.
GEOCHEMISTRY AND REACTION PATH MODELING OF THE BEOWAWE HYDROTHERMAL SYSTEM, NEVADA: A BARREN END-MEMBER EPITHERMAL SYSTEM
Presented by Mark Leatherman
A candidate for the degree of Master of Science
And hereby certify that in their opinion it is worthy of acceptance
ACKNOWLEDGEMENTS
I would like to thank Carol Nabelek for her assistance with the ICP-AES analysis at the
University of Missouri—Columbia. Many thanks go to my colleagues Dr. Albert Hofstra and Dr.
Donald Sweetkind of the United States Geological Survey-Denver, and Dr. Mark Person and
Amlan Banerjee at the New Mexico Institute of Mining and Technology. Particular thanks go to
Dr. Kevin Shelton and Dr. Baolin Deng for their valuable reviews that have contributed significant improvement of this manuscript.
Many thanks go to my advisor, Dr. Martin Appold, for his patience, expertise, encouragement, and wisdom for the various twists and turns the research process underwent.
Special thanks go to my wife, Rebecca, who has greatly helped me along the way, as well as the rest of my family.
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TABLE OF CONTENTS
ACKNOWLEDGEMENTS………………………………………………………………………….ii
LIST OF FIGURES………………………………………………………………………………….iv
LIST OF TABLES………………………………………………………………………………...... v
ABSTRACT…………………………………………………………………………………………vi
I. INTRODUCTION………………………………………………………………………1
II. GEOLOGIC BACKGROUND………………………………………………………....7
III. ICP-AES ANALYSIS………………………………………………………………...13
IV. FLUID INCLUSION MICROTHERMOMETRY…………………………………....17
V. GEOCHEMICAL REACTION PATH MODELING…..…………………………….24
i. COLE-RAVINSKY PROFILE (CR) MODEL………..………………..24
A. SEGMENT 1……………………………………………………….28
B. SEGMENT 2……………………………………………………….30
C. SEGMENT 3……………………………………………………….37
D. SEGMENT 4……………………………………………………….40
E. SEGMENT 5……………………………………………………….41
F. SEGMENT 6……………………………………………………….44
ii. PERSON ET AL. PROFILE (P) MODEL……………………………....46
iii. HIGH S MODEL………………………………………………………..52
VI. DISCUSSION.………………………………………………………………………..55
VII. CONCLUSIONS……………………………………………………………………...62
VIII. REFERENCES………………………………………………………………………..64
IX. APPENDIX I………………………………………………………………………….67
X. APPENDIX II………………………………………………………………………...73
XI. APPENDIX III………………………………………………………………………..90
XII. APPENDIX IV………………………………………………………………………107
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LIST OF FIGURES
Figure Page
1. Fumarole Photo………………………………………………………………………...2
2. Map of Field Area……………………………………………………………………...3
3. Sinter Terrace Photo………………………………………………………………...... 4
4. Stratigraphic Column……………………………………………………………….....8
5. Alteration Profile…………………………………………………………………...... 10
6. Hand Sample Photos…………………………………………………………………12
7. ICP-AES Trends…………………………………………………………………...... 16
8. Fluid Inclusion Photos…………………………………………………………….....18
9. Microthermometry Histograms………………………………………………………22
10. Conceptual Model-Cross Section………………………………………………...... 27
11. pH-Fugacity-TDS Data………………………………………………………….....32
12. CR Model Mineral Precipitation Data……………………………………………..33
13. CR Model Aqueous Concentration Data…………………………………………..34
14. CR Model Precious Metal-Porosity-Hydraulic Conductivity Data………………..35
15. P Model Aqueous Concentration Data………………………………………….....47
16. P Model Mineral Precipitation Data…………………………………………….....48
17. P Model Precious Metal-Porosity-Hydraulic Conductivity Data……………….....49
18. High S Model Data………………………………………………………………...53
19. Precious Metal Stability Plots……………………………………………………..57
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LIST OF TABLES
Table Page
1. ICP-AES Data………………………………………………………………………...14
2. Microthermometry Data………………………………………………………………19
3. Initial Fluid Parameters……………………………………………………………….25
4. Spece8 Mineral Saturation States…………………………………………………….29
5. Hydrologic-Theoretical Ore Grade Calculations…………………………………...... 59
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ABSTRACT
The Beowawe geothermal field in north-central Nevada is one of the hottest and
most active in the Basin and Range province of the western U.S. Prior to disturbances of
the field caused by geothermal power exploration and development beginning in 1959,
and culminating with the completion of a 16.7 MW power plant in 1986, Beowawe had
more active geyser activity than any other site in North America outside of Yellowstone
National Park. The Beowawe area also contains characteristics of low-sulfidation
epithermal, Au-Ag deposits including sinter deposits, banded chalcedony veins with
adularia, bladed calcite, slotted quartz pseudomorphs after calcite, pyrite, and discharging
low chlorinity fluid that is neutral to basic in pH. Despite these characteristics, Beowawe
appears to be only weakly mineralized with respect to gold and silver. Although
Beowawe is one of the hottest areas in the Great Basin, there is no evidence for a magma
body at depth.
Regional fluid flow is apparently channeled along the NNW- and ENE-striking
Muleshoe and Malpais faults, which serve as recharge and discharge pathways,
respectively. Numerical modeling suggests that rapid advection of meteoric recharge had
cooled the fluid-flow system to a near uniform temperature of <150°C about 5000 years
ago. This contrasts with the 70-80°C/km temperature gradients that are currently
observed at Beowawe. In addition, the amount of silica that could have been deposited
under predicted model conditions in 5000 years is far less than what is observed in the
field. Together, these observations suggest that fluid flow at Beowawe occurred
episodically over a much longer period of time, perhaps on the order of hundreds of
thousands of years. The purpose of this study was to look for evidence of episodic flow
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in the sinter and vein deposits, and to use reaction-path modeling to determine if a
hydrothermal fluid sourced from a deep carbonate reservoir could produce mineral
alteration assemblages observed in the field and ore grade precious metal mineralization
along its ascent to the surface.
Stratigraphically-controlled Samples of Beowawe sinter from several different
stratigraphic levels were analyzed by ICP-AES. None of these samples showed
detectable quantities of Au and Ag, which is probably due to the low solubility of gold in
the discharging fluids. Elements that did exist in detectable concentrations include Li
(0.46-46 ppm), S (2.3-4900ppm), Fe (49-18,000 ppm), Zn (0.3-76 ppm), As (6.2-60
ppm), Ba (12-230ppm), and Tl (20-29ppm). The heterogeneous variation in sinter compositions supports episodic fluid flow with fluctuating composition rather than a progressive evolution in fluid composition as a result of cooling. Fluid inclusion microthermometry performed on sinter and vein samples indicate silica was precipitated from dilute fluids that ranged from 0 to 1.4 eq. wt.% NaCl, which is quite similar to current discharged waters at Beowawe. The fluid inclusions have highly variable homogenization temperatures that probably reflect heterogeneous entrapment of liquid and vapor in a geyser environment. Geochemical reaction-path modeling of fluid sourced from a hypothesized deep carbonate aquifer ascending along the Malpais Fault supports current discharge fluid chemistry, and observed alteration mineral assemblages.
The modeling predicts precious metal mineralization to be weak overall, but most concentrated at depths of >1700 m and at shallower depths of <400 m. The modeling predicted variable net mineral precipitation along the ascent path, from which porosity
and permeability change were calculated. The calculations showed that enough flow
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episodes could occur before the porosity was fully occluded and the flow system would
shut down to allow ore grade precious metal mineralization to occur along some intervals
of the flow path.
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INTRODUCTION
The Beowawe geothermal field in north-central Nevada is one of the hottest and most active in the Basin and Range province of the United States. Prior to disturbances of the field caused by geothermal power exploration and development beginning in 1959, and culminating with the completion of a 16.7 MW power plant in 1986, Beowawe had more active geysering than any other site in North America outside of Yellowstone National Park (White, 1998).
Although geyser activity at Beowawe has now ceased, several fumaroles (Figure 1) and hot springs still exist.
The Beowawe geothermal area is located within the Whirlwind Valley watershed of the
Shoshone Range (Figure 2). Outcroppings of Tertiary volcanic rocks bound the valley as the
Argenta Rim on the north and as the Malpais Rim on the south. Hydrothermal fluids discharge
along the fault scarp of the ENE-striking Malpais Rim at temperatures ranging from 57 to 98⁰C.
Fluid temperatures increase sharply to about 230° C at three kilometers below the surface (Smith,
1983; Rimstidt & Cole, 1983; Struhsacker, 1986). Discharging hydrothermal fluids are dilute, with total dissolved solids (TDS) contents ranging from about 900 to 1400 ppm consisting
predominantly of sodium, sulfate, bicarbonate, and silica. The fluids tend to be slightly to
moderately basic, with pH ranging from about 7 to 9 (Cole & Ravinsky, 1984; Rimstidt & Cole
1983; White, 1998; Day, 1987). Over time, the discharging hydrothermal fluids have deposited a
massive siliceous sinter terrace (Figure 3) that is approximately 1.6 km long, 1 km wide, and 65 m thick and estimated to contain about 1.28 × 1011 kg of silica (Rimstidt & Cole, 1983).
The anomalously high fluid temperatures at Beowawe raise the question of how the fluids
acquired their heat, given the absence of any evidence for concurrent magmatism. Support for
the amagmatic character of the hydrothermal system lies in the absence of any surficial igneous
rocks younger than 10 Ma (Coolbaugh et al., 2005), low 3He/4He ratios in the hydrothermal fluids
(White, 1998), and the meteoric hydrogen and oxygen isotope composition of the hydrothermal
1
Figure 1: Photograph of an active fumarole at Beowawe (note hammer for scale).
2
3
Figure 3: Photograph of the siliceous sinter terrace (white) formed by hydrothermal fluid discharge at Beowawe. Note the road going up along the lower right-hand side of the terrace for scale.
4 fluids (John et al., 2003). In addition, Person et al. (2008) have recently completed a numerical model of groundwater flow and heat transport along a 60 kilometer cross section across the
Shoshone Range and adjacent basins. Their work showed that groundwater entering the subsurface along the Argenta Rim could have descended along the Muleshoe fault until it reached karsted Paleozoic carbonates at a depth of several kilometers, whereupon it moved laterally before ascending back to the surface along the Malpais fault. The model predicted a high temperature-depth gradient with fluid reaching a temperature of 240° C at a depth of three kilometers within the first few hundred years after the onset of flow that is consistent with present-day observations (Smith, 1983; Olmsted & Rush, 1987). However, after only about 1600 years, the temperature gradient along the Malpais fault had become nearly uniform due to high rates of advective heat transport, and absolute fluid temperatures were progressively decreasing with time. Mass balance calculations show that this period of time is too small to deposit the amount of silica that is present in the Beowawe sinter terrace (Rimstidt & Cole, 1983), leading
Person et al. (2008) to conclude that hydrothermal fluid flow and silica deposition have occurred in multiple brief episodes each on the order of 1000’s of years or less in duration, on an overall time span of hundreds of thousands of years. One objective of the present study was to look for geochemical evidence of episodic fluid flow in the Beowawe silica deposits.
The Beowawe geothermal area also has many characteristic features of low-sulfidation epithermal Au-Ag deposits such as fault-controlled fluid flow, siliceous sinter deposits, bladed calcite replaced by silica, sulfides coexisting with banded chalcedony and adularia, and fluid discharge that is dilute and neutral to basic in pH. The area is however only weakly mineralized with respect to gold and silver. Struhsacker (1986) has documented a low grade Au-Ag-As anomaly centered on White Canyon, an area of silica veining located about 1.5 km east of the sinter terrace that may be an earlier product of the Beowawe hydrothermal system. Surface samples and drill hole cuttings from depths up to ~100 m commonly had gold concentrations on the order of 10’s to 100’s of ppb, with a maximum of 560 ppb. The gold tends to be most
5 concentrated in sulfide-bearing margins of chalcedony veins. Silver anomalies are less widespread than gold, but reach a higher maximum concentration of 15 ppm. The maximum arsenic concentration found was 484 ppm. Struhsacker (1986) speculated about the reasons for the weak gold-silver mineralization and suggested that it was a result of the amagmatic character of the hydrothermal system, high permeability of the Malpais fault, and low gas contents in the fluids that prevented overpressuring and episodic hydrothermal eruption (steam explosions) and
brecciation. A second major objective of the present study was to investigate further the reasons
for the weak gold-silver mineralization at Beowawe by modeling the solubility and reactivity of
gold and silver in a hypothetical hydrothermal fluid as it ascended from a deep carbonate aquifer
to the surface.
6
GEOLOGIC BACKGROUND
The Beowawe geothermal field is located on the southwestern margin of Whirlwind
Valley at the intersection of the NNW-trending Northern Nevada Rift and the NE-trending
Shoshone Range (Figure 2). The Northern Nevada Rift is a result of Basin and Range extension, which stretches from near the Nevada-Oregon-Idaho border to southeast Nevada (John et al.,
2000). The rift is Middle Miocene in age and is thought possibly to reflect the passage of the
Yellowstone hot spot through northern Nevada during that time (John et al. 2003). The rift is exposed in the Argenta and Malpais Rims, two forks of the Shoshone Range that were uplifted between the Late Miocene and the Quaternary as a result of Basin and Range extension that form the northern and southern boundaries of Whirlwind Valley, respectively (Faulder et al., 1997;
John et al., 2003). Most of the hydrothermal discharge at Beowawe occurs at the base of the
Malpais Rim, apparently focused along the Malpais fault scarp. Additional hydrothermal fluid
focusing may have been caused by the NNW-trending Dunphy Pass fault, which parallels the
Northern Nevada Rift boundary and intersects the Malpais fault near Beowawe.
The stratigraphy of the Beowawe area is shown in Figure 4. The deepest rocks identified
are autochthonous early Paleozoic carbonates that lie approximately 3 to 5 km below the ground
surface (Zoback, 1979; Olmsted & Rush, 1987). These rocks may have undergone karst
dissolution and served as an important reservoir for circulating hydrothermal fluids. The
carbonate rocks are overlain by rocks of the Roberts Mountain thrust. The stratigraphically
lowest and thickest member of the thrust package is the Ordovician Valmy Formation, which
consists of at least 1700 m of predominantly siliciclastic rocks. In the Beowawe area, the Valmy
Formation consists mainly of gray to red siliceous siltstones that can grade into quartzite, with
lesser amounts of conglomerate, chert, chalcedony, sandstone, and shale (Zoback, 1979). Active
Paleozoic tectonics have significantly fractured this formation allowing the intrusion of Tertiary
diabase dikes (Struhsacker, 1980; Cole & Ravinsky, 1984). The Valmy Formation is
7
Figure 4: Simplified stratigraphic column of the Whirlwind Valley area of Beowawe.
8 unconformably overlain by about 45 to125 m of felsic tuffaceous sediments dated to be Late
Eocene in age, and interbedded by hornblende biotite lavas (Struhsacker, 1980). The sediments consist of clasts of the Valmy Formation, and felsic and mafic volcanic rocks in a matrix of feldspathic sand and quartz, feldspar, glass, and mafic mineral pyroclasts, largely cemented with calcite. Overlying the tuffaceous sediments are about 1200 m of Middle Miocene volcanic rocks.
The rocks consist predominantly of basaltic andesite and pyroxene dacite with lesser basalt, tuff, and tuffaceous sedimentary rock (Struhsacker, 1980; Zoback, 1979; Cole & Ravinsky, 1984).
These volcanic rocks are prominently exposed in the Argenta and Malpais Rims. Overlying the volcanic rocks in Whirlwind Valley are several tens of meters of Tertiary and Quaternary gravel, landslide, and alluvium deposits. These deposits are primarily clastic weathering products of the
Tertiary volcanic rocks and Valmy Formation.
Figure 5 shows how hydrothermal fluid flow at Beowawe has produced a zoned alteration of the host rocks to a depth of at least 2800 m (Struhsacker, 1980; Rimstidt & Cole,
1983; Cole & Ravinsky, 1984). Listed in order of increasing depth, zone I is characterized by zeolite, zone II by smectite, zeolite, and enrichment of Au, zone III by smectite, chlorite, and enrichments of Zn, Au, Ag, and Hg, and zone IV by chlorite, epidote, and enrichments of Zn, Cu,
Ag, and As (Figure 5a). The presence of some alteration minerals at temperatures lower than expected thermodynamically based on the present-day thermal profile, and the presence of hematite in the upper three alteration zones led Cole & Ravinsky (1984) to suggest that the
Beowawe hydrothermal system is currently in a state of thermal collapse (Figure 5b). In this scenario, a hot, reducing sodium chloride-fluid that dominated the system earlier is being progressively displaced by a cooler, more neutral, oxidizing sodium-bicarbonate-sulfate fluid.
Significant hydrothermal alteration is also observed in the rocks of White Canyon, located about 1.5 km east of the Beowawe sinter terrace. This discharge site is now inactive, possibly indicating that the locus of hydrothermal activity has shifted westward over time. The mineral alteration assemblage at White Canyon consists of multi-colored banded chalcedony with
9
Figure 5: (a) Major hydrothermal alteration zones as a function of depth for the Beowawe area, including prominent element anomalies within each zone (after Cole & Ravinsky, 1984). (b) Alteration mineral distribution and intensity (H = high, L = low) with depth. The solid curved line marks the measured thermal profile of Beowawe whereas the dashed curve is a reference boiling temperature for pure water (after Cole & Ravinsky, 1984).
10 adularia, slotted-habit calcite replaced by quartz (Figure 6), and minor pyrite with dark red and gray friable sulfides. Struhsacker (1986) suggested that hydrothermal fluids at White Canyon eventually precipitated enough silica to seal up most proximal open space. However, the permeability of the Malpais fault west of White Canyon was high enough to allow fluid flow to shift to its present location at Beowawe. The absence of brecciation at White Canyon supports this interpretation, indicating the presence of permeable flow conduits that prevented fluid pressure build-up and resultant steam explosions.
The hydrology of the Beowawe area has been studied by Day (1987), Olmsted & Rush
(1987), Faulder et al. (1997), and Person et al. (2008). The present day water table slopes
downward from west to east across Whirlwind Valley toward the Humboldt River. Groundwater
recharge is focused in the uplands bordering the western end of Whirlwind Valley. Faults such as
the Muleshoe Fault appear to channel much of the recharge to kilometer-scale depths, allowing
groundwater to reach the high observed discharge temperatures observed at Beowawe. Much of
the descending groundwater is likely to be intercepted by porous and permeable, possibly karsted carbonates immediately underlying the Roberts Mountains thrust, where the groundwater is temporarily sequestered and equilibrates with its host rock before ascending to the surface via the
Malpais Fault. This conclusion is supported by the Beowawe discharge waters’ light oxygen and hydrogen isotope composition, which has been interpreted to reflect a meteoric source of
Pleistocene age, unexpectedly old given Person et al.’s (2008) modeling prediction that groundwater can traverse the hypothesized flow path on the order of 100’s of years, and the waters’ heavy carbon isotope composition and high bicarbonate to chloride ratios, which indicate greater interaction with carbonate rocks than siliciclastic rocks (Zoback, 1979; Mariner et al,
1983; Day, 1987). On the basis of electric self-potential data, Zoback (1979) has inferred the existence of a second, smaller reservoir at an approximate depth of one kilometer, possibly created by increased fracturing from the intersection of the range front faults with the Northern
Nevada Rift graben-bounding faults.
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Figure 6: Hand samples of bladed calcite replaced by quartz (top), and banded chalcedony- adularia from White Canyon (bottom).
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ICP-AES ANALYSIS
Geochemical evidence for the episodicity of the Beowawe hydrothermal system was sought by measuring the bulk composition of siliceous sinter from twelve discrete stratigraphic positions in the sinter terrace. All of the samples were analyzed using inductively coupled plasma-atomic emission spectroscopy (ICP-AES) in the Department of Geological Sciences at the
University of Missouri—Columbia. Samples were prepared for analysis by powdering 0.2 g of material and heating it at 1,050°C for 30 minutes to drive off volatiles. The ashed samples were then mixed with 1.5 mL of 3% HF solution in separate Teflon bombs and heated in a 1400 W microwave oven at low power for 20 minutes to break silicate bonds. To aid in the dissolution of metals, 1 mL of 4% aqua regia was added to each sample solution and heated for ten minutes in a microwave oven at low power. Fifteen mL of 30% boric acid solution were then added to each sample solution followed by 10 more minutes of low power heating in a microwave oven to break up any fluoride complexes that may have formed by secondary reactions. The final step consisted of diluting the sample solutions to 50 mL with deionized water. An accompanying acid blank was prepared using the above procedure for instrument calibration, along with three other check standard solutions. These three standards were used to calibrate the instrument with intensities of
0.1 mg/l, 1.0 mg/l, and 10 mg/l. Elements chosen for analysis were based on the reported composition of Beowawe discharge waters from Cole & Ravinsky (1984), Day (1987), Rimstidt
& Cole (1983), and White (1998) as well as typical low-sulfidation alteration assemblages which included Li, S, Fe, Cu, Zn, As, Se, Mo, Ag, Sb, Te, Ba, Au, Tl, and Pb.
Elemental concentrations determined from the ICP-AES analyses and detection limits are shown in Table 1. The elements that registered above their detection limits in every sample were
Fe, Ba, and As with concentrations ranging from 113 to 17,800 ppm, 13.2 to 225 ppm, and 6.17 to 60 ppm, respectively. The elements that registered below their detection limits in every sample analyzed included Au, Ag,
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Table 1: Minor and trace element composition of Beowawe sinter samples as determined by ICP-AES.
ICP-AES Concentrations (ppm) Sample ID Elevation (ft.) Li S Fe Zn As Ba Tl B11 1,667 46.3 1,120 17,800 17.5 60.0 45.4 ---- B10 1,554 18.4 4,480 803 ---- 7.26 225 ---- B9 1,568 ------103 ---- 14.0 19.0 ---- B8 1,538 14.3 ---- 551 6.36 12.8 50.8 ---- B7 1,538 6.73 27.4 1,780 ---- 8.6 95.7 ---- B6 1,538 5.17 ---- 113 3.1 11.6 13.2 14.0 B5 1,568 ------349 ---- 14.8 15.5 29.1 B4 1,557 10.9 226.0 764 75.5 6.71 89.9 ---- B3 1,565 2.33 ---- 358 12.5 8.98 52.1 19.8 B2 1,488 18.2 184.0 6,880 30.0 9.11 148.0 ---- B-1c 1,488 12.4 9.97 2,540 7.62 9.84 97.9 ---- B-1b 1,488 19.2 30.5 4,820 ---- 6.17 177.0 ----
“----“indicates that the concentration of the element in the sample was below the detection limit.
*Detection limits for the analyzed elements are as follows: 0.2 ppm for Tl, 0.09 ppm for Pb, 0.08 ppm for Se, 0.05 ppm for As, 0.04 ppm for Te, 0.03 ppm for Sb and Au, 0.02 ppm for S, 0.01 ppm for Li, Fe, Cu, Mo and Ag, 0.004 ppm for Zn, and 0.001 ppm for Ba.
14
Cu, Se, and Mo. Maximum concentrations found for the remaining elements were 46.3 ppm for
Li, 4,880 ppm for S, 75.5 ppm for Zn, and 29.1 ppm for Tl.
The elements Li, S, Fe, Zn, As, and Ba existed in detectable concentrations in enough sinter samples to allow trends to be sought as a function of elevation (Figure 7). Although concentrations can vary considerably within stratigraphic horizons, with the exception of As, all of the elements show a general pattern of decreasing concentration from an elevation of about
1490 to 1540 m, increasing concentration from about 1540 to 1555 m, decreasing concentration from about 1555 to 1560 or 1570 m and increasing concentration about 1560 or 1570 to 1667 m.
The pattern of As concentration with elevation is largely antithetical to that of the other elements.
The interpretation of these elemental concentration patterns is equivocal, but given the mineralogical homogeneity of the sinter terrace as a function of elevation, variations in sinter composition could plausibly reflect variations in parent hydrothermal fluid composition. This would indicate that hydrothermal fluid composition at Beowawe was not constant over time, which is consistent with the episodic fluid flow proposed by Person et al. (2008).
None of the elements detected is particularly enriched in the Beowawe sinter compared to average continental crust (Taylor and McLennan, 1985), with the exception of As, which is enriched by about an order of magnitude, and Tl, which when detected is enriched by about two orders of magnitude. Thus, the Beowawe hydrothermal fluid did not appear to have had strongly mineralizing character when it discharged at the surface, though it was capable of strong mineralogical alteration at greater depths.
15
Figure 7: Concentrations of Li, S, Fe, Zn, As, and Ba in the Beowawe sinter terrace as a function of elevation, as determined by ICP-AES. The solid line in each plot indicates the trend of variation of the concentrations. At elevations where more than one sinter sample was analyzed, the trend line connects to the mean value of the measurable concentrations.
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FLUID INCLUSION MICROTHERMOMETRY
In order to understand more of the fluid temperature and salinity history of the Beowawe hydrothermal system, microthermometry was performed on fluid inclusions hosted by opaline sinter from Beowawe, and on quartz-chalcedony-adularia veins from within and extending eastward from White Canyon. The microthermometry was conducted using a Linkam THGMS
600 heating-cooling stage in the Department of Geological Sciences at the University of
Missouri--Columbia. A total of 60 fluid inclusions, half from older White Canyon veins and half from younger opaline sinter, were analyzed. Petrographic observations showed quartz replacements of bladed calcite not to contain any usable fluid inclusions. All of the fluid inclusions analyzed are considered to be primary, based on the criteria of Goldstein & Reynolds
(1994). Inclusions found in White Canyon vein quartz display a prismatic to ovoidal habit with an average liquid-vapor ratio of 7:1 whereas those found in younger siliceous sinter tend to possess irregular, spicule-type habits with an average liquid-vapor ratio equaling 4.5:1 (Figure 8).
For each sample chip, homogenization temperatures for all fluid inclusions were recorded before last-ice-melting temperatures so as not to risk stretching the inclusions, which would cause falsely elevated homogenization temperatures. In addition, because heating can also cause fluid inclusion stretching, liquid-vapor ratios were always compared to original, pre-microthermometry photographs of the fluid inclusions once the first homogenization temperature measurement in a sample chip had been performed to ensure that no changes in liquid-vapor ratio had occurred and that subsequent homogenization temperature measurements in the sample chip were accurate.
Microthermometry results are displayed in Table 2 and in Figure 9. Most of the fluid inclusions in the samples were composed of a single liquid water phase. The remainder consisted of liquid and vapor in highly variable proportions. No daughter minerals were observed in any of the fluid inclusions. Petrographic assemblages of liquid-vapor fluid inclusions of clear primary origin and sizes large enough for microthermometry analysis were rare in the samples studied.
17 a) b)
c)
Figure 8: (a) Primary fluid inclusion assemblages oriented along growth bands in vein quartz from White Canyon, and consisting mostly of liquid-only fluid inclusions. (b) Possible assemblage of randomly oriented fluid inclusions lacking any clear association with growth features in quartz vein host from White Canyon. Most of the fluid inclusions in the photograph consist of a single liquid aqueous phase, with the exception of a two-phase aqueous liquid-vapor fluid inclusion visible in the center. (c) Large, two-phase, spicule-shaped fluid inclusion hosted by opaline sinter from Beowawe. Note characteristic banding of sinter matrix.
18
Table 2: Fluid inclusion microthermometry data from White Canyon silica veins and Beowawe siliceous sinter.
Sample ID Inclusion ID Sample Dimensions Th (°C) Tm (°C) Eq. Wt.% NaCl Type (µm) Qtz.-chal.- EVBV-1 1-1 adul. vein 7 3 129.4 −0.4 0.72 Qtz.-chal.- EVBV-1 1-2 adul. vein 5.5 3.5 255.0 0 0 Qtz.-chal.- EVBV-1 1-3 adul. vein 5.25 3 100.0 0 0 Qtz.-chal.- EVBV-1 1-1 adul. vein 8.5 3.25 127.3 −0.4 0.72 Qtz.-chal.- EVBV-1 1-2 adul. vein 4 4.5 211.7 0 0 Qtz.-chal.- EVBV-1 1-1 adul. vein 6 3.5 135.6 0 0 Qtz.-chal.- EVBV-2 1-2 adul. vein 4.5 3 155.7 0 0 Qtz.-chal.- EVBV-2 1-3 adul. vein 12.5 6.25 147.9 0 0 Qtz.-chal.- EVBV-2 1-4 adul. vein 5.25 3.25 158.7 0 0 Qtz.-chal.- EVBV-2 1-5 adul. vein 9.5 7.5 144.6 0 0 Qtz.-chal.- WCBV-1 1-1 adul. vein 5.25 4.25 163.7 0 0 Qtz.-chal.- WCBV-1 1-1 adul. vein 4.25 2 187.3 −0.1 0.18 Qtz.-chal.- WCBV-1 1-2 adul. vein 5 4 192.5 −0.1 0.18 Qtz.-chal.- WCBV-1 1-3 adul. vein 10.25 10.25 167.3 0 0 Qtz.-chal.- WCBV-1 2-1 adul. vein 6.5 5.5 126.0 −0.1 0.18 Qtz.-chal.- WCBV-2 2-2 adul. vein 4.5 2.5 158.3 −0.1 0.18 Qtz.-chal.- WCBV-2 2-3 adul. vein 7.5 5.25 186.3 −0.1 0.18 Qtz.-chal.- WCBV-2 2-4 adul. vein 5.25 4.5 197.8 0 0 Qtz.-chal.- WCBV-2 2-5 adul. vein 9 3.75 138.7 −0.5 0.90 Qtz.-chal.- WCBV-2 2-6 adul. vein 9 3.5 109.3 −0.2 0.36 Qtz.-chal.- WCBV-2 2-7 adul. vein 6.75 3.25 162.1 0 0 Qtz.-chal.- WCBV-2 2-8 adul. vein 8.75 2.5 140.6 −0.1 0.18
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Sample ID Inclusion ID Sample Dimensions Th (°C) Tm (°C) Eq. Wt.% NaCl Type (µm) Qtz.-chal.- WCBV-2 2-9 adul. vein 4.5 3 123.5 0 0 Qtz.-chal.- WCBV-2 2-10 adul. vein 6 3 167.9 0 0 Qtz.-chal.- WCBV-2 3-1 adul. vein 8 3 166.2 −0.3 0.54 Qtz.-chal.- WCBV-2 3-2 adul. vein 5 2 148.8 −0.4 0.72 Qtz.-chal.- WCBV-2 4-1 adul. vein 5.5 5.5 130.5 −0.2 0.36 Qtz.-chal.- WCBV-2 4-2 adul. vein 5.75 3.5 118.2 −0.6 0.36 Qtz.-chal.- WCBV-2 1-1 adul. vein 9 6 146.8 −0.2 0.36 Qtz.-chal.- WCBV-2 1-1 adul. vein 7 3.5 185.6 0 0 Opaline BEO-ST-2 1-2 sinter 22.5 19.5 183.2 −0.2 0.36 Opaline BEO-ST-2 1-3 sinter 11 4.25 143.4 0 0 Opaline BEO-ST-2 1-4 sinter 22 12.5 162.8 −0.1 0.18 Opaline BEO-ST-2 1-5 sinter 17 12.75 228.6 −0.2 0.36 Opaline BEO-ST-7 2-1 sinter 7 5.25 178.2 −0.1 0.18 Opaline BEO-ST-7 2-2 sinter 9.5 6 181.7 −0.1 0.18 Opaline BEO-ST-7 2-3 sinter 7.75 2.25 190.0 0 0 Opaline BEO-ST-7 1-1 sinter 9.75 4.25 169.3 0 0 Opaline BEO-ST-7 2-1 sinter 5 3.75 171.1 −0.2 0.36 Opaline BEO-ST-7 2-2 sinter 110 61 218.6 0 0 Opaline BEO-ST-7 2-3 sinter 8.5 8.5 188.5 0 0 Opaline BEO-ST-7 2-4 sinter 14 12.25 249.3 −0.3 0.54 Opaline BEO-ST-11 3-1 sinter 12 8.5 134.6 −0.8 1.45 BEO-ST-11 Opaline 3-2 sinter 6 4.25 229.6 −0.3 0.54 BEO-ST-11 Opaline 3-3 sinter 7.75 4.5 294.9 0 0 BEO-ST-11 Opaline 3-4 sinter 6.5 6.5 250.1 −0.4 0.72
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Sample ID Inclusion ID Sample Dimensions Th (°C) Tm (°C) Eq. Wt.% NaCl Type (µm) BEO-ST-11 Opaline 3-5 sinter 5 5 313.1 0 0 BEO-ST-11 Opaline 3-6 sinter 8.5 5 194.4 −0.2 0.36 BEO-ST-11 Opaline 3-7 sinter 7.5 5 174.1 0 0 BEO-ST-11 Opaline 1-1 sinter 13.5 2 200.7 0 0 BEO-ST-11 Opaline 1-2 sinter 6.5 4.75 201.5 −0.1 0.18 BEO-ST-11 Opaline 1-3 sinter 7.5 7.5 219.8 −0.3 0.54 BEO-ST-11 Opaline 2-1 sinter 9.5 4.75 233.6 0 0 BEO-ST-11 Opaline 2-2 sinter 11 5 213.1 −0.2 0.36 Opaline BEO-ST-12 1-1 sinter 6 6 160.2 0 0 Opaline BEO-ST-12 1-2 sinter 10.25 5 188.9 0 0 Opaline BEO-ST-12 1-3 sinter 5.75 2.75 263.7 −0.1 0.18 Opaline BEO-ST-12 2-1 sinter 11.25 9.75 165.8 0 0 Opaline BEO-ST-12 2-2 sinter 32 20.5 159.0 0 0 Opaline BEO-ST-12 3-1 sinter 16.75 6.75 209.1 0 0
* “Qtz.-chal.-adul. Vein” corresponds to Quartz-chalcedony-adularia vein.
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a)
b)
Figure 9: Microthermometry histograms displaying homogenization (Th) temperatures (a), and melting-point depression (Tm) temperatures (b) of White Canyon vein quartz and Beowawe siliceous sinter.
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Most of the microthermometry data are from isolated fluid inclusions, though some are from fluid inclusion arrays that appear to correlate with growth bands (Figure 8a). Homogenization temperatures (Th) for liquid-vapor fluid inclusions have a wide range of values from 100 to
313°C, with a standard deviation of ±1°C, indicative of heterogeneous liquid-vapor entrapment typical of geyser environments (Figure 9a). Fluid inclusions hosted by unconsolidated sinter have a higher average Th of 205°C compared to fluid inclusions hosted by White Canyon quartz veins, whose Th averages about 159°C. Last-ice-melting temperatures (Tm) for fluid inclusions hosted
by both sinter and quartz veins are consistently at 0°C with a minimum of −0.8°C, with a
standard deviation of ±0.1°C (Figure 9b). These temperatures indicate low total dissolved solids
contents corresponding to 0 to 1.4 equivalent weight % NaCl.
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GEOCHEMICAL REACTION PATH MODELING
Geochemical reaction path modeling was carried out to investigate the behavior of hydrothermal fluid as it ascended along the Malpais Fault from a deep carbonate reservoir underlying the Roberts Mountains thrust fault. Three scenarios were modeled. The first model simulated a fluid that cooled as it ascended according to the present-day thermal gradient reported by Cole & Ravinsky (1984) for the Ginn 1-13 well. The second model simulated a fluid that cooled much less as it ascended, following the thermal gradient during peak heat transport predicted by the hydrologic modeling of Person et al. (2008). In this second scenario, fluid discharges at the ground surface at a temperature of 96° C in contrast to a temperature of 25° C in the first scenario. The third model simulated the effects of elevated sulfur concentration on precious metal transport and precipitation under the present-day thermal gradient.
Cole-Ravinsky profile (CR) model
The first model tracks the evolution of a hydrothermal fluid as it rises along the present- day geothermal gradient in the Ginn 1-13 well, and thus provides insights into the reaction products formed during waning hydrothermal activity. The initial composition of the model fluid