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Geochemical analysis of thermal fluids from southern Mount Meager, British Columbia,
Canada
Katherine Huang
Faculty of Earth Sciences
University of Iceland
2019
Geochemical analysis of thermal fluids from southern Mount Meager, British
Columbia, Canada
Katherine Huang
60 ECTS thesis submitted in partial fulfillment of a
Magister Scientiarum degree in Geology
MS Committee
Andri Stefánsson
Master’s Examiner
Snorri Guðbrandsson
Faculty of Earth Sciences
School of Engineering and Natural Sciences
University of Iceland Reykjavik, May 2019
Geochemical analysis of thermal fluids from southern Mount Meager, British Columbia,
Canada
Mount Meager Thermal Fluids Geochemical Analysis
60 ECTS thesis submitted in partial fulfillment of a Magister Scientiarum degree in
Geology
Copyright © 2019 Katherine Huang
All rights reserved
Faculty of Earth Sciences
School of Engineering and Natural Sciences
University of Iceland
Sturlugata 7
101, Reykjavik
Iceland
Telephone: 525 4000
Bibliographic information:
Katherine Huang, 2019, Geochemical analysis of thermal fluids from southern Mount
Meager, British Columbia, Canada, Master’s thesis, Faculty of Earth Science, University
of Iceland, pp. 92.
Printing: Háskólaprent Ltd
Reykjavik, Iceland, May 2019
Abstract
Geothermal exploration has been ongoing intermittently in the Mount Meager geothermal
area, British Columbia, Canada, since the 1970s. However, a geochemical interpretation of
the many fluid samples collected during this time period has not been carried out for several
decades, leaving gaps in understanding of the system which modern techniques can help fill.
Thermal fluids from springs and wells in the southern Mount Meager geothermal field were
analyzed to understand the fluid origin, controls on chemistry from effects of mixing and
water-rock interaction, and to determine the reservoir temperature and composition.
Chloride and boron concentrations ranged from 100 to 3300 ppm and 0.3 to 28 ppm,
respectively. These very high conservative element concentrations cannot alone be explained
by rock dissolution and are instead likely supplied by a single magmatic source. Calculated
reservoir compositions suggest that select deep wells have experienced significant CO2
degassing from reservoir to the surface, and high SO4 content present from surface samples
is traced down to the reservoir. These data corroborate the hypothesis that a magmatic
component exists and contributes to B, Cl, CO2 and SO4 fluid composition, although CO2
and SO4 may have alternate sources. Select geothermometers calculated reservoir
temperatures of up to 283 °C for central deep wells and as low as 30 °C and 5 °C for hot
springs and cold springs, respectively. Like many high-temperature geothermal systems, the
compositions of thermal fluids appeared to be controlled by the equilibrium between the
fluid and observed secondary minerals. Hot springs and wells on the eastern and northern
sides of the reservoir are of low temperature and likely define the boundaries of peripheral
waters. Wells to the southeast contained anomalously high Cl and SO4, suggesting a possible
magmatic input of these components which may be controlled by the east-west running
Meager Creek Fault Zone. There is a significant source of hot, Cl- and CO2-rich thermal
waters supplying deep wells MC-1, MC-2, MC-6 and MC-8, and possibly MC-3. These
NaCl waters likely define the high temperature, central location of the geothermal reservoir.
Útdráttur
Á Mount Meager jarðhitasvæðinu í Bresku-Kólumbíu, Kanada, hefur síðan á áttunda
áratugnum staðið yfir könnun á jarðhita þar, þó með hléum. Á þessu tímabili hefur miklum
fjölda vökvasýna verið aflað en þau hafa hingað til ekki verið túlkuð með aðferðum
jarðefnafræðinnar. Slík túlkun getur aukið skilning á jarðhitasvæðinu töluvert, sér í lagi með
nýjum jarðefnafræðilegum aðferðum sem þróaðar hafa verið síðustu áratugina.
Jarðhitavökvi úr náttúrulegum uppsprettum og borholum á suðurhluta jarðhitasvæðisins var
rannsakaður til að skorða betur uppruna vökvans, skoða áhrif blöndunar og samspil vatns og
bergs á efnafræði vökvans og greina samsetningu og hitastig djúpvökvans. Klór-styrkur
mældist á bilinu 100 til 3300 ppm og bór-styrkur 0.3 til 28 ppm. Háan styrk þessara efna er
ekki hægt að útskýra eingöngu með uppleysingu bergs en benda frekar til þess að vökvarnir
séu upprunnir úr kviku. Reiknuð samsetning djúpvökvans bendir til að í sumum borholunum
hafi átt sér stað mikil afgösun CO2, frá djúpvökva til yfirborðs og að háan styrk SO4 í
yfirborðssýnum megi rekja til djúpvökvans. Þessi gögn styðja þá tilgátu að djúpvökvinn eigi
sér uppruna að hluta í kviku, sem eykur hlut B, Cl, CO2 og SO4 í vökvanum, þótt CO2 og
SO4 í vökvanum gætu komið úr fleiri uppsprettum. Valdir jarðhitamælar gefa allt að 283°C
reiknað hitastig djúpvökva í borholum miðsvæðis, allt niður í 30°C fyrir hveri og 5°C fyrir
kaldar uppsprettur. Líkt og mörg háhitasvæði virðist samsetning jarðhitavökvans stýrð af
jafnvægi milli vökvans og síðsteinda sem koma fram. Hverir og borholur á austur- og
norðurhluta svæðisins skilgreina sennilega vatnaskil. Borholur á suðausturhluta svæðisins
eru óvenju rík af Cl og SO4, sem bendir til mögulegs kvikuuppruna þessara efna sem
mögulega er stýrt af Meager Creek misgengjabeltinu. Það er töluvert magn af heitum, Cl- og
CO2-ríkum jarðhitavökva sem streymir í borholur MC-1, MC-2, MC-6 og MC-8 og
mögulega MC-3. Þessi Na-Cl vötn skilgreina líklega miðju háhitadjúpvökvans.
vii
Table of Contents
List of Figures ................................................................................................................... viii
List of Tables ....................................................................................................................... ix
Acknowledgements ............................................................................................................. xi
1 Introduction ................................................................................................................... 13
2 Study area ...................................................................................................................... 15 Hydrology .............................................................................................................. 16 Geothermal activity ............................................................................................... 19
2.2.1 Previous work on fluid geochemistry .......................................................... 19
3 Database ......................................................................................................................... 25
4 Data handling ................................................................................................................ 29 Data filtering.......................................................................................................... 29
Estimation of fluid origin and mixing using conservative element behavior ........ 31
Reservoir fluid composition, reservoir temperature, aqueous speciation, and
mineral saturation .................................................................................................. 32 Distribution of geothermal activity ....................................................................... 34
5 Chemical characteristics of samples ........................................................................... 39
6 Discussion ...................................................................................................................... 41 Fluid origin and mixing using boron and chloride systematics............................. 41
Reservoir temperature and fluid composition ....................................................... 44 6.2.1 Fluid-mineral interaction ............................................................................. 48
Distribution of geothermal activity ....................................................................... 51
7 Conclusions .................................................................................................................... 55
References........................................................................................................................... 57
Appendix A ......................................................................................................................... 65
Appendix B ......................................................................................................................... 75
Appendix C ......................................................................................................................... 85
viii
List of Figures
Figure 2.1 Left: Geomorphological belts of the Canadian Cordillera (after Harris et al.,
1997). Right: The Mount Meager Volcanic Complex (in yellow box) sits
at the intersection of the Pemberton and Garibaldi Belts (Lewis & Souther,
1978). ................................................................................................................ 15
Figure 2.2 Geological map showing the volcanic assemblages of the MMVC (adapted
from Proenza, 2012). ........................................................................................ 17
Figure 2.3 Hot springs and previously drilled wells in the southern reservoir of the
MMVC (adapted from Proenza, 2012; GeothermEx, 2005). ........................... 18
Figure 4.1 Calculated percentage ion balance plotted against select element
concentrations. Dotted lines are interpreted intrumental detection limits.
Red indicates data point from a sample of M12-80D, black indicates data
point from a sample of MC-2. .......................................................................... 30
Figure 5.1 Piper plot of all sampled waters. ........................................................................ 40
Figure 6.1 The relationship between (A) B and Cl and (B) Cl/B molal ratio and Cl for
the thermal waters. Precipitation content is plotted along with average
compositions of andesite and basalt. Progressive rock leaching (ξ) from
0.01 to 1 is also graphed ................................................................................... 43
Figure 6.2 Comparison of different geothermometers. ....................................................... 45
Figure 6.3 CO2 and SO4 composition of all waters from sampling (blue) and for wells
using reservoir composition calculated from WATCH. ................................... 47
Figure 6.4 Activities of major cations as a function of temperautre. The solid line
shows logK for each reaction. .......................................................................... 50
Figure 6.5 Distribution of key variables Cl, CO2, SO4, and temperature. ........................... 54
ix
List of Tables
Table 2.1 Geothermometry results from past literature vary between source and
geothermometer used. Temperatures are in °C. ............................................... 21
Table 3.1 Overview of database. .................................................................................... 26-27
Table 4.1 Summary of lithologies encountered during well drilling. .................................. 32
Table 4.2 Composition of sources that are considered to be contributing Cl and B to
the geothermal waters. Cl and B are in ppm. .................................................... 32
Table 4.3 Equations for geothermometers used. Concentrations are in mg/kg. T is in
°C. ..................................................................................................................... 36
Table 4.4 Balanced reactions used to calculate loqQ. ......................................................... 37
Table 6.1 Temperatures ranges for all geothermometers for each well and hot spring
type. .................................................................................................................. 44
Table 6.2 Range of concentrations for reservoir compositions of samples that
degassed. ........................................................................................................... 46
Table 6.3 Averages and standard devations of reservoir Cl, CO2, SO4 and temperature
for sample locations. Concentrations are in ppm; temperatures are in °C. ...... 52
xi
Acknowledgements
My greatest thanks goes to Andri Stefánsson for his seemingly infinite knowledge on fluid
geochemistry and geothermal energy. I am grateful for his patience, guidance, help, and for
everything I’ve learned, and I hope to one day have a fraction of his wisdom. Thank you to
Jóhann Gunnarsson Robin for help with WATCH and to my peers in Iceland for sharing
interest and love of geology, volcanology, geothermal energy, and geochemistry. I am also
grateful for my family and for my partner Michael for the support during my time here in
Iceland.
I could not have written this thesis without the projects and research previously conducted
over many decades. I appreciate all of the work that was done before my time, as well as the
pioneers who have been pushing for geothermal energy in Canada- I can only hope that this
research may contribute. Finally, I would like to thank my dear friend Sally Innis, for I would
not be studying geology today without her.
13
1 Introduction
Geochemical composition of thermal fluids may be used to understand fluid origin, mixing
between two or more fluid sources, degree of water-rock interaction, and to estimate
reservoir temperature and composition. As such, geothermal geochemistry is one of the key
tools applied in geothermal exploration (Arnórsson & D'Amore, 2000).
Among the key questions that arise when considering the utilization of geothermal resources,
as well as their general nature, is the origin of the water itself. Stable and radiogenic isotopes
and conservative elements have been studied to address these questions in the past. The
pioneering work by Craig (1961, 1963) and Friedman et al. (1964) and later, for example
Árnason (1976, 1977) led to the extensive work on stable hydrogen and oxygen isotopes of
cold and geothermal waters and precipitation. Conservative elements such as boron and
chloride have also been applied to trace water sources and degree of mixing of two or more
water types, and also to assess water-rock interaction (Arnórsson & Andrésdóttir, 1995). In
meteoric source water, their concentrations are usually low and, upon water-rock interaction
and mixing with for example seawater, the elemental concentrations and relative ratios
change. These changes can, in turn, be used to quantify the various sources of the two
elements.
Studies of alteration mineralogy and fluid composition in geothermal systems show that
equilibrium is closely approached between the geothermal fluids and secondary minerals
formed in the systems except for mobile elements such as chloride and boron (e.g.,
Giggenbach 1981, 1988; Arnórsson 1983a; Pang & Reed 1998; Stefánsson & Arnórsson,
2000). Such mineral-fluid equilibria provides the basis for application of calculating
reservoir temperatures using solute and gas geothermometry. Solute geothermometers
include quartz (Arnórsson et al., 1983a; Fournier, 1977; Fournier & Potter; 1982),
chalcedony (Arnórsson et al., 1983b; Fournier, 1977), and the cations such as Na-K
(Arnórsson et al., 1983b; Fournier, 1979a; Giggenbach, 1988; Tonani, 1980; Truesdel,
1976), K-Mg (Giggenbach, 1988), Na-K-Ca (Fournier & Truesdel, 1973), Na-K-Ca Mg
(Fournier & Potter, 1979) and Na-Li (Fouillac & Micard, 1981). Univarient
geothermometers, such as quartz and chalcedony, are based on single element concentrations
and may be subject to secondary changes upon boiling, fluid mixing, and condensation.
Ratio chemical geothermometers like Na-K overcome this challenge by using element ratios
that are affected to the same degree by these secondary processes. They are, however, limited
by equilibrium and rate conditions. Many of the geothermometers vary in the temperature
ranges that they operate in based on mineral-solution equilibrium systematics and therefore
the appropriate geothermometer(s) must be selected for the geothermal system being studied.
Numerous fluid geochemistry studies have been carried out for thermal fluids in the Mount
Meager geothermal field as part of earlier exploration programs. Chemical analysis of the
hot springs and/or well fluids have been published by Hammerstrom and Brown (1977),
Adams et al. (1985), Ghomshei et al. (1986), Adams and Moore (1987), Ghomshei and Clark
(1993), and Grasby et al. (2000). Chemical analyses of reservoir rocks and drill core have
been published by Moore et al. (1983), Moore et al. (1985), and Adams and Moore (1987)
to reconstruct the hydrothermal events in the system. Stable and radioactive isotope data
14
have been studied by Clark et al. (1982), Ghomshei and Clark (1993), Phillips (1994), and
Clark and Phillips (2000). Despite the number of publications on thermal fluid geochemistry
in the area, there is still uncertainty about the temperature and characteristics of the
geothermal reservoir. Presently, researchers agree that the geothermal system in general is
composed of NaCl fluids, while fluid flow is limited by low permeability throughout the
reservoir. However, there is debate about the fluid origin and amount of mixing within the
system. Some research presents evidence of mixing between brine and non-thermal
groundwaters (Ghomshei et al., 1986; Ghomshei & Clark, 1993), while others suggest that
there is no indication of mixing (Adams et al., 1985; Adams & Moore, 1987). As a
geochemical analysis of the 200+ fluid samples has not been carried out in 30 years,
reviewing the data with modern programs and present knowledge of thermal fluid
geochemistry may provide more insight on the geothermal system.
Here, the aim is to use existing data to classify the origin of the geothermal waters, to
understand the controls on water chemistry and the effects of mixing and water-rock
interaction, and to calculate the reservoir temperatures of the southern Mount Meager
geothermal reservoir. Due to lack of geochemical fluid data in the north reservoir, this
research focuses on the south reservoir where most of the deep wells have been drilled.
Reservoir fluid temperatures and compositions were estimated using geothermometry and
geochemical modeling, respectively. In addition, conservative elemental relations were used
to assess the source and mixing of fluids. Together, these results help to construct an overall
model of the geothermal system to support future geothermal development at Mount Meager.
15
2 Study area
The Canadian Cordillera in western Canada is composed of five geomorphological belts:
The Insular Belt, Coast Belt, Intermontane Belt, Omineca Belt, and Foreland Belt. The
Pleistocene to Recent Mount Meager Volcanic Complex (MMVC) within the Coast Plutonic
Belt sits 150km north of Vancouver, British Columbia (Figure 2.1) (Read, 1977). The
complex is transected by the north-northwest trending plutonic Pemberton Belt and the
north-south trending Garibaldi Belt composed of Quaternary volcanoes. Both belts are
associated with subduction of the Juan de Fuca plate (Lewis & Souther, 1978).
Figure 2.1 Left: Geomorphological belts of the Canadian Cordillera (after Harris et al.,
1997). Right: The Mount Meager Volcanic Complex (in yellow box) sits at the intersection
of the Pemberton and Garibaldi Belts (Lewis & Souther, 1978).
The MMVC is dominantly calc-alkaline and made up of assemblages composed of andesite
and dacite flows, basaltic lava flows and pyroclastic deposits, dacite domes and flows, and
pyroclastic units, all which lie unconformably on a basement of plutonic (granitic to quartz
diorite) and metamorphic rocks (Stasiuk & Russell, 1989; Read, 1977)Error! Reference
source not found.. These units are shown on the geological map in Figure 2.2. The
assemblages are products of around 2.2 My of intermittent volcanic activity (Read, 1977,
1990). The initial eruption was explosive and gas-rich, which fractured the basement; it has
been postulated that this caused the basement to seal itself, creating a geothermal reservoir
(Lewis & Souther, 1978). The uppermost assemblage is the Pebble Creek formation
16
(formerly Bridge River Ash Assemblage), composed of eruptive products of lava domes,
flows, and rhyodacite volcaniclatics from the most recent 2350 B.P. ±140 years eruption
(Stasiuk et al., 1996; Hickson et al., 1999; Stewart, 2002; Stewart et al., 2003; Nasmith et
al., 1967; Clague et al., 1995).
The complex is cut by numerous steeply dipping faults thought to be of crustal magnitude
(NSBG, 1974). The Meager Creek Fault Zone is a northeast-dipping normal fault that runs
east-west along Meager Creek. The exact size is unknown, but it is postulated to be the major
conduit for ascending geothermal fluids in the area. Several smaller faults run perpendicular
to this fault, including the No Good Discontinuity, the Camp Fault, and the Carbonate Fault.
The No Good Discontinuity is a north-south striking, east-dipping fault interpreted to bisect
the volcanic complex along a linear zone of volcanic vents. The Camp Fault is a northeast-
striking, nearly-vertical dipping fault (NSBG, 1981). The Carbonate Fault dips away from
the reservoir and is thought to control the flow of cool water to the carbonate springs (NSBG,
1980). The faults are shown on the geological map in Figure 2.2.
Hydrology
Hydrology research has been published by Moore et al. (1985) and Adams and Moore
(1987), and reported by NSBG (1980) and GeothermEx (2004). Geothermal waters originate
from the quartz diorite basement and occupy permeable fractures and faults (NSBG, 1980).
NSBG (1980) noted that large volumes of fluid loss during shallow well drilling indicate
high permeability in the basement rock. However, permeability in the upper portions of the
reservoir is low, which limits fluid flow above basement rock (Moore et al., 1985).
Petrographic, mineralogical, and trace element studies by Adams and Moore (1987) have
established that upward movement of geothermal fluids in the reservoir is focused by fault
and fracture zones, steeply dipping dikes, and hydrothermal breccias related to recent
volcanic activity.
Because there is disagreement regarding fluid mixing, there is no universally accepted
conceptual hydrology model for the Mount Meager geothermal system. However,
temperature and chemical data provide relatively clear boundaries of the reservoir. The No
Good Discontinuity or nearby Carbonate Fault is likely the western temperature boundary
of the system. Chemical evidence and temperature measurements suggest either that the No
Good Discontinuity is the boundary, featuring a downflow zone or that the Carbonate Fault
is the boundary that circulates flowing water upward (GeothermEx, 2004; NSBG, 1980).
The southern boundary is still poorly defined but is postulated to be the Meager Creek Fault
Zone along Meager Creek (NSBG, 1980). Thermal fluids from wells MC-1 and MC-2 are
likely part of an upflow and outflow zone which flows south to feed into hot springs along
Meager Creek (GeothermEx, 2004). Slimwells drilled in between the deep wells show
evidence of convection of high temperature fluids at shallow depths; this area is possibly in
the center of the geothermal reservoir anomaly (GeothermEx, 2004).
17
Figure 2.2 Geological map showing the volcanic assemblages of the MMVC (adapted from Proenza, 2012).
18
Figure 2.3 Hot springs and previously drilled wells in the southern reservoir of the MMVC (adapted from Proenza, 2012; GeothermEx, 2005).
19
Geothermal activity
Six hot spring complexes lie within the general north-northwest trend of the Pemberton Belt
within the Canadian Cordillera (Lewis & Souther, 1978). Hot and cold springs in this area
originate from the basement rock (Read, 1977). Among these spring complexes are the
Meager Creek Hot Springs, Placid Hot Springs, and No Good Warms Springs which all lie
along Meager Creek on the southeast edge of the MMVC and discharge chemically similar
water at 20-55 ºC (Clark et al., 1982). Water from these springs are thought to be related to
recent volcanic activity (Lewis & Souther, 1978).Carbonate and siliceous sinters appear in
surface deposits at Meager Creek Hot Springs and other hot springs south along Meager
Creek, while white carbonate deposits are found around the CaCO3 Cold Springs (Moore et
al., 1985).
2.2.1 Previous work on fluid geochemistry
The hot springs on the southeast end of the MMVC (Placid Hot Springs, Meager Creek Hot
Springs, and No Good Warm Springs) are all Na-Cl dominated, oversaturated in amorphous
silica, and are thought to be recharged from meteoric water locally on the volcanic complex
and mixed with older thermal water. Stable isotope and Cl- data analysis however, suggest
that thermal waters from Meager Creek Hot Springs originate from mixing between cold
groundwater and MC-1 water (Gomshei & Clark, 1993). Based on He isotope data, the
mixing ratio of cold water to MC-1 thermal water could be approximately 2:1 (Clark &
Phillips, 2000).
Isotope and major element analyses contradict these mixing models, suggesting that thermal
water from MC-1 and hot springs, although likely all originate from meteoric water, are
chemically and isotopically distinct (Adams et al., 1985; Adams & Moore, 1987). Piper plots
and TDS with isotope analyses show three distinct water groups: Moderate TDS NaCl waters
with large isotope shifts (MC-1), low TDS NaCl waters with small isotope shifts (Meager
Creek Hot springs), and high TDS NaCl waters with moderate isotope shifts (shallow wells
and other springs). The difference in TDS as well as isotope shifts between MC-1 and
Meager Creek Hot Springs waters suggests separate histories of deep, subvolcanic fluid flow
and shallow fluid flow, respectively. Thermal waters from shallow wells and other springs
are possibly cooled geothermal fluid with a long residence time. Overall, the data suggest
the geothermal reservoir is composed of multiple small geothermal systems with few faults
and fracture systems limiting the degree of mixing.
Early studies by Hammerstrom and Brown (1977) analyzed hot spring and shallow well
chemistry. Based on distribution of species calculations, the thermal waters appear to be in
equilibrium with near-surface alteration assemblages. Similarly, constant ion concentration
ratios published by Ghomshei et al. (1985) suggest that the reservoir is in thermochemical
equilibrium and has experienced fluid mixing. They propose that well MC-1 is fed by a
single brine which experienced either steam loss or mixing with cold, NaCl fresh water.
GeothermEx (2004) proposes yet another model that features five distinct groups of water
with various mixing patterns. The first group is represented by unmixed MC-1 and MC-2
NaCl waters. In this area, deep, 200 °C NaCl water is overlain by 50-130 °C Na-SO4-HCO3
20
waters, which does not mix with other waters. Near-surface NaCl waters interact with cold
groundwater and this mixture presents at the surface. To the west, MC-3 and MC-5 waters
are rich in Na-SO4 and NaHCO3 with lower and variable concentrations of Cl. GeothermEx
(2004) proposes that the deep NaCl water in this area mixes with the overlying Na-SO4-
HCO3 waters, creating Na-SO4, HCO3, NaCl surface waters. Bicarbonate waters exist on the
periphery of the deep wells in wells M2 and M6 formed from mixing of CO2-rich gas with
groundwater. These carbonate springs are thought to represent the lateral margins of the
geothermal system. A fourth group of shallow wells and cold springs exists even further
from the deep wells. The fluid compositions plot closely to MC-5 fluids on the Cl-SO4-HCO3
ternary diagram, but concentrations of components are significantly higher. This suggests
that this area is composed of cool, saline waters with a history of high temperature. Finally,
the No Good Warm Springs, Placid Hot Springs, and Meager Creek Hot Springs all have
similar fluid compositions which suggest mixing of NaCl waters from MC-1 and MC-2 with
Na-SO4-Na-HCO3 waters and groundwater.
The source of fluids from deep wells is still unknown, and much of the past research was
conducted before wells MC-6, MC-7, and MC-8 were drilled. Therefore, current knowledge
of the deep system is mostly based on data from MC-1. He isotopes indicate a possible
volcanogenic input of He (Phillips, 1994; Clark & Phillips, 2000). High PCO2 values,
enriched δ13CDIC, elevated 3He/CO2 ratios, and elevated Cl- may be explained by subduction
of Juan de Fuca plate sediments and pore water (Clark & Phillips, 2000).
Multiple studies have been published with geothermometry calculations for hot springs and
wells. Results are summarized in Table 2.1.
21
Table 2.1 Geothermometry results from past literature vary between source and geothermometer used. Temperatures are in °C.
Source Geothermometer Meager Creek MC-1 MC-2 MC-3 MC-5
Clark et al., 1982 Mg-corrected Na-K-Ca 105
Gomshei et al., 1984 Silica 200-210
Silica (steam loss) 185-195
Na/K 180-200
Adams and Moore (1987) Na/Li 280
Na-K-Ca(-Mg) 50-70 190
Grasby et al., 2000 Amorphous Silica 60
Quartz 184
Chalc 163
Na/K 222
Na-K-Ca 188
Mg/Li 87
GeothermEx, 2004 Silica 190-205 190-205 230-235 230-235
22
Chemical analyses of reservoir rocks and drill core have been published by Moore et al.
(1983), Moore et al. (1985), and Adams and Moore (1987) to understand the hydrothermal
events in the system. Analyses of core and cuttings suggest that the area has been affected
by at least two hydrothermal events. The older event is characterized by chalcopyrite
mineralization and propylitic alteration of the crystalline basement (Moore et al., 1983). The
younger event characterized by volcanic activity less than 2 My ago, resulted in secondary
mineral assemblages in dikes and breccias and in the crystalline basement. Alteration in the
dikes and breccias is predominantly characterized by distributed sheet silicates, including
smectite, chlorite, illite, saponite, and talc. Assemblages of epidote, K-feldspar, and
actinolite were found at depths below 1625m. Veins of carbonate ± quartz ± hematite as well
as sulfide deposits (mainly pyrite) were sporadically distributed. Many fractures in the upper
portion of the reservoir were infilled with carbonate during hydrothermal brecciation and
fluid boiling, which may contribute to the reservoir’s low permeability (Moore et al., 1985).
The crystalline basement of mainly meta quartz diorite was also highly altered with smectite
and illite, as well as kaolinite. Other secondary minerals included chlorite, Fe-Ti oxides,
epidote, and carbonate, the latter predominately present as veins in the upper 1800m of the
rock. Veins of quartz, hematite, and silicate minerals including epidote, chlorite, K-feldspar,
actinolite, and biotite were also found at depths below 700m. Many of these assemblages
cannot be distinguished between pre- and post-volcanic activity, although the sheet silicates
in the basement are certainly post-volcanic products. Within both the dikes/breccias and the
basement, four distinct alteration zones define the secondary mineral assemblages and their
respective temperature ranges (e.g. Muffler & White, 1969; Elders et al., 1979; McDowell
& Elders, 1980; Bird et al., 1984). The upper smectite zone is normally found in geothermal
areas which have experienced temperatures of 50-175 °C while the interlayered illite-
smectite zone is normally formed in the range of 150-225 °C. The illite and chlorite
assemblage is formed above 200 °C, but can exist at temperatures as low as 150 °C. Finally,
the epidote zone and the actinolite, biotite, and talc zone form in geothermal systems at >200-
250 °C and >300 °C, respectively.
A 1970s energy crisis spurred an onset of geothermal exploration in British Columbia,
sponsored by the federal government and the government-owned utility company, BC Hydro
(Ghomshei et al., 2004). Initial exploration included geophysical and geochemical
exploration and temperature gradient/slimhole drilling in the north and the south Meager
areas. In the early 1980s, three deep exploration wells, MC-1, MC-2, and MC-3 were drilled
to depths of approximately 3500 m in south Meager, as well as several more shallow
slimwells. The deep wells were targeted to a significant low resistivity anomaly, but
insufficient detailed information on subsurface geometry caused them to miss the target. The
wells encountered temperatures up to 270 ºC at 300 m, but all three lacked permeability. By
1982, three deep wells and 19 temperature gradient/slimhole wells had been drilled.
The project halted in 1985 due to financial cutbacks, and in 1989 the geothermal lease at the
Meager site was transferred to Meager Creek Development Corp., a subsidiary of Western
GeoPower Corp. Work finally resumed in the early 1990s when MC-5 was drilled. After
drilling, work halted again until 2000, when Western GeoPower Corp. extended work to the
north (Ghomshei et al., 2004). A 2001 MT survey placed the low resistivity anomaly much
further north, towards Pylon Peak extending to the north of Meager Creek. The next three
wells, M17, M18, and M19 targeted this anomaly and were drilled at much higher elevations
in 2001-2002. High temperature gradients encountered in the wells corroborated the MT
data. In 2002, Western GeoPower Corp. drilled deep wells MC-6, MC-7, and MC-8 to target
23
an inferred upflow zone to the north of Meager Creek. Drill collar locations, bottomhole
projections, and hot springs are show in Figure 2.3. Of the 19 temperature gradient/slimhole
wells drilled, only M1-74, M2-75D, M7-79D, and M12-80D had complete fluid analyses
(explained in Chapter 4) and therefore are the only wells included in maps and analyses. For
simplification, they are labelled on maps as M1, M2, M7, and M12, respectively.
25
3 Database
Hot spring geochemistry data has been collected and published by Souther (1976), NSBG
(1975, 1980), Hammerstrom and Brown (1977), Michael and Fritz (1979), Shenker (1980),
and Clark et al. (1980). Fluid chemistry from wells has been published by NSBG (1975,
1980, 1981), Hammerstrom and Brown (1977), Michael and Fritz (1979), Shenker, (1980),
Clark et al. (1980), BC Hydro (1983), and Western GeoPower Corp. (2009). Results were
compiled recently by Proenza (2012).
In the south reservoir, data are available from a total of 251 fluid samples from three
hot/warm springs, three cold springs, six shallow wells, and five deep wells. Shallow and
deep well depths range from 45-899 m and 2380-3606 m, respectively. For each sample
location, there was at least one samples that analyzed the major elements SiO2, Na, K, Ca,
Mg, Cl, SO4 and C as HCO3, CO3, and/or CO2. Other components analyzed varied between
samples and included Fe, Mn, F, B, Li, As, and NH4. An overview of what has been analyzed
is shown in Table 3.1.
From these compiled sources, only the data that met the selection criteria outlined in the
following section were used.
26
Table 3.1 Overview of database.
Name Type Count Depth (m) Source Elements Analyzed
Meager Creek
Hot Springs Hot Spring 11 Surface
NSBG, 1975; NSBG, 1980;
Hammerstrom & Brown, 1977;
Michael & Fritz, 1979; Shenker,
1980; Clark et al., 1980
SiO2, Na, K, Ca, Mg, Cl, SO4, HCO3, Fe, Mn,
F, B, Li
Placid Hot
Springs Hot Spring 1 Surface Clark et al., 1980 SiO2, Na, K, Ca, Mg, Cl, SO4, HCO3, Fe, Mn
No Good
Warm Spring Hot Spring 9 Surface
NSBG, 1975; Hammerstrom &
Brown, 1977; Shenker, 1980;
Clark et al., 1980
SiO2, Na, K, Ca, Mg, Cl, SO4, HCO3, Fe, Mn,
F, B, Li
Boundary Cold
Springs
Cold
Spring 1 Surface Clark et al., 1980 SiO2, Na, K, Ca, Mg, Cl, SO4, HCO3, Fe, Mn
CaCO3 Springs Cold
Spring 6 Surface
NSBG, 1975; Clark et al., 1980;
Shenker, 1980
SiO2, Na, K, Ca, Mg, Cl, SO4, HCO3, Fe, Mn,
F, B, Li
Problem Cold
Spring
Cold
Spring 1 Surface Clark et al., 1980 SiO2, Na, K, Ca, Mg, Cl, SO4, HCO3, Fe, Mn
EMR-1 Shallow
Well 9 45
NSBG, 1975; Hammerstrom &
Brown, 1977; Michael & Fritz,
1979; Shenker, 1980; Clark et al.,
1980
SiO2, Na, K, Ca, Mg, Cl, SO4, HCO3, Fe, Mn,
F, B, Li
M1-74D Shallow
Well 6 347.5
NSBG, 1975; Michael & Fritz,
1979; Clark et al., 1980
SiO2, Na, K, Ca, Mg, Cl, SO4, HCO3, Fe, Mn,
F, B, Li
M2-75D Shallow
Well 2 774 NSBG, 1975; Clark et al., 1980 SiO2, Na, K, Ca, Mg, Cl, SO4, HCO3, Fe, Mn
M7-79D Shallow
Well 1 899 NSBG, 1981
SiO2, Na, K, Ca, Mg, Cl, SO4, HCO3, CO3, Fe,
Mn, F, B, Li
(Continued)
27
Table 3.2 Overview of database (continued).
M12-80D Shallow
Well 2 605 NSBG, 1981
SiO2, Na, K, Ca, Mg, Cl, SO4, HCO3,
CO3, Fe, Mn, F, B
MC-1 Deep Well 145 3040 BC Hydro, 1985 SiO2, Na, K, Ca, Mg, Cl, SO4, CO2, NH4,
F, B, As, Li
MC-2 Deep Well 20 3605.6 BC Hydro, 1985 SiO2, Na, K, Ca, Mg, Cl, SO4, CO2, NH4,
F, B, As, Li
MC-3 Deep Well 26 3503 BC Hydro, 1985 SiO2, Na, K, Ca, Mg, Cl, SO4, CO2, NH4,
F, B, As, Li
MC-6 Deep Well 6 2662 Western GeoPower Corp. 2009 SiO2, Na, K, Ca, Mg, Cl, SO4, HCO3,
CO3, B
MC-8 Deep Well 3 2380 Western GeoPower Corp. 2009 SiO2, Na, K, Ca, Mg, Cl, SO4, HCO3, F,
B
29
4 Data handling
Handling of the fluid chemistry data involved three steps:
(1) Filtering of available data from the literature
(2) Estimation of fluid origin and mixing using conservative element behavior
(3) Calculation of reservoir fluid composition, estimation of reservoir temperature,
calculation of aqueous speciation and mineral saturation indices
For the third step, the calculations were done with the aid of the WATCH program
(Arnórsson et al., 1982) version 2.4 (Bjarnason, 2010) as well as the PHREEQC program
and the WATEQ database (Parkhurst and Appelo, 2013).
Data filtering
The available data on fluid composition were filtered based on data quality and extent of
elements analyzed. First, samples with an incomplete set of data that did not include the
major elements Si, Na, K, Ca, Mg, Cl, SO4, and HCO3 were removed for consideration.
Second, the overall quality of the chemical analysis were assessed from the percentage ion
balance (% IB) defined by the formula,
%IB = ∑ 𝑚𝑖
+𝑧𝑖+ − |∑ 𝑚𝑖
−𝑧𝑖−|
∑ 𝑚𝑖+𝑧𝑖
+ + |∑ 𝑚𝑖−𝑧𝑖
−|× 100
(1)
where 𝑚𝑖+ and 𝑚𝑖
− are the 𝑖𝑡ℎ aqueous species molal concentrations and 𝑧𝑖+ and 𝑧𝑖
− are the
𝑖𝑡ℎ charges for cations and anions, respectively. The ion balance calculations were carried
out with the aid of the PHREEQC program at the temperature of each pH measurement.
The results were plotted as a function of total elemental concentration (Figure 4.1). As
observed, samples with low element concentrations had higher percentage errors, which
follows the general relationship of increased errors of the chemical analysis with decreasing
concentration. At concentrations above the instrumental detection limits, which were
estimated from the plots, samples with outliers over ±10% IB error were removed. Only two
samples, one from well M12-80D and one from well MC-2, were contributing to high %IB
above instrumental detection limits for most elements.
Of the 251 available fluid samples, 200 samples were included in the final table after data
filtering. Their chemical compositions are given in Appendix A.
30
Figure 4.1 Calculated percentage ion balance plotted against select element
concentrations. Dotted lines are interpreted intrumental detection limits. Red indicates
data point from a sample of M12-80D, black indicates data point from a sample of MC-2.
31
Estimation of fluid origin and mixing using
conservative element behavior
Typically, water stable isotopes (δD and δ18O) have been applied to establish the origin of
the geothermal water and assess mixing behaviour. Such water isotope data are currently not
available for geothermal fluids at Mount Meager, therefore, conservative element analysis
was instead used. Conservative elements including Cl and B have been studied to trace the
origin of geothermal waters (Truesdell, 1975; Arnórsson et al., 1989; Giggenbach,
1991; Arnórsson & Andrésdóttir, 1995) and mixing between non-thermal and geothermal
waters (Ellis, 1970; White, 1970; Arnórsson; 1970, Stefánsson & Arnórsson, 1975;
Fournier, 1977, 1979b, 1985; Truesdell, 1991). Boron and Cl are considered to be
incompatible during weathering and low-temperature geothermal alteration of most rocks,
meaning that they generally do not precipitate once added to the fluid phase (e.g., Arnórsson
& Andrésdóttir, 1995). The sources of B and Cl in geothermal waters may be considered to
be the source water including seawater and meteoric water, rock leaching, and magma
degassing. These elements originate from sea spray in precipitation, directly from seawater
filtering through the groundwater systems. The boron and chloride composition of seawater
is well established (Bruland, 1983) and meteoric water (precipitation) closely follows the
B/Cl seawater ratio (Arnórsson & Andrésdóttir, 1995). Upon water-rock interaction (water
dissolving the rock), the water becomes more enriched in B relative to Cl and the reaction
will continue until the Cl/B ratio reaches that of the rock. These elements are therefore able
to trace water source(s) and assess the effects of progressive water-rock interaction and
mixing ratios between different water sources.
In order to assess the various boron and chloride sources and their contributions to the waters,
data on chemical composition of precipitation and rocks are needed. No such data are
available for rocks at Mount Meager or local precipitation. Lithological units encountered
during well drilling are summarized in Table 4.1 and indicate that, although there is high
variability in lithology, the most common rock unit is quartz diorite. Past literature has also
described meta quartz diorite as the major rock component of the area (Adams & Moore,
1987). Therefore, quartz diorite was taken as a proxy for the host rock of the thermal fluids.
The chemical composition of precipitation in Canada is highly variable, ranging from Cl
concentration of <0.1 to >10 ppm (e.g., Rutherford, 1967; Aherne et al., 2010) and following
Arnórsson and Andrésdóttir (1995) B/Cl ratio in precipitation may be assumed to follow that
of seawater and the B concentration of precipitation can be estimated from the respective
elemental seawater ratio and Cl concentration in precipitation. Chloride and B
concentrations of andesite, the aphanitic form of diorite, have been measured at around 200-
300 ppm and 17-20 ppm, respectively (Sanchez, 1993; Gméling et al., 2005). The upper
concentrations of andesite are used in this study to show the maximum amount of chloride
and boron that the host rock can contribute to the thermal waters. Basalt composition was
also plotted for comparison, using theoleiite Cl and B compositions of 170 ppm and 1.2 ppm,
respectively (Arnórsson & Andrésdóttir, 1995). A summary of the range of B and Cl rocks,
seawater/precipitation used in this study is listed in
Table 4.2.
32
Table 4.1 Summary of lithologies encountered during well drilling.
Well From (m) To (m) Lithology
EMR-1 17 45 Quartz Diorite
M1-74D 124 347 Gneissic Quartz Diorite
M2-75D 11 91 Gneissic Quartz Diorite
M7-79D 26 120 Gneissic Quartz Diorite, Quartz Diorite, Faults
120 168 Feldspar Porphyry with Faults
168 367 Gneissic Quartz Diorite, Quartz Diorite, Rhyolite,
Feldspar Porphyry
M12-80D 14 605 Quartz Diorite with Andesite and Dacite Dykes
and shear zones near surface
MC-1 30 2000 Amphibolite- Quartz Diorite with Dykes
2000 3041 Quartz Diorite with Pyroxene Basalt Diabase
Dykes
MC-2 0 1215 Quartz Diorite with Dykes
1215 3503 Gneiss with Dykes
MC-3 30 3500 Quartz Diorite with Dykes
MC-6 400 1600 Quartz Diorite
1600 2400 Gneiss
2400 2663 Hornblende Biotite and Quartz Diorite
MC-8 400 1500 Quartz Diorite with Volcanic/Andesite Dikes
1500 2380 Gneiss
Table 4.2 Composition of sources that are considered to be contributing Cl and B to the
geothermal waters. Cl and B are in ppm.
Contributor Cl B Cl/B Molal Ratio Source
Seawater 1330 Arnórsson and Andrésdóttir,
1995
Rainwater 0.1-10 <0.0023 1330 Rutherford, 1967; Aherne et
al., 2010
Andesite 200 20 3.05 Sanchez, 1993
Basalt 170 1.2 43 Arnórsson and Andrésdóttir,
1995
Reservoir fluid composition, reservoir
temperature, aqueous speciation, and
mineral saturation
The WATCH speciation program of Arnórsson et al. (1982), version 2.4 (Bjarnason, 2010),
was used to calculate the component concentrations in the reservoir fluid for the present
study. For these calculations, the chemical compositions of samples from non-thermal and
33
sub-boiling wells was taken to represent the compositions of the waters in the producing
reservoir. On the other hand, water samples collected from the two-phase wells (vapour and
liquid) and boiling hot springs are not representative of the parent reservoir water, since
boiling and degassing have modified the chemical composition from the reservoir to surface.
The WATCH program uses data on water and steam samples collected at the surface to
calculate the reservoir fluid composition. In the case of unavailable steam data, steam loss
and gas (CO2 and H2S) partitioning can be estimated assuming the reservoir and sample
collection temperatures to be known. For these calculations, boiling was taken to be adiabatic
(isolated thermodynamic system) and no steam was assumed to be present in the reservoir
beyond the zone of depressurization boiling. It follows that steam fraction (𝑋𝑣) at sampling
is calculated from the equation,
𝑋𝑣 =ℎ𝑟𝑒𝑠 − ℎ𝑠,𝑙𝑞
ℎ𝑠,𝑣 − ℎ𝑠,𝑙𝑞
(2)
where ℎ𝑟𝑒𝑠 is the enthalpy of the reservoir fluid taken to be equal to liquid enthalpy at the
reservoir temperature and ℎ𝑠,𝑣 and ℎ𝑠,𝑙𝑞 are the vapour and liquid enthalpies at the sampling
temperature, respectively. Following, the reservoir fluid 𝑖𝑡ℎ elemental concentrations are
calculated using conservation of mass,
𝑚𝑖𝑟𝑒𝑠 = 𝑋𝑣𝑚𝑖
𝑠,𝑣 + (1 − 𝑋𝑣)𝑚𝑖𝑠,𝑙𝑞
(3)
where 𝑚𝑖𝑟𝑒𝑠 is the 𝑖𝑡ℎ elemental reservoir concentration, and 𝑚𝑖
𝑠,𝑣 and 𝑚𝑖
𝑠,𝑙𝑞 are the respective
concentrations in the sampled vapor and liquid phases.
It follows that, in order to calculate the reservoir fluid composition from data of wells and
spring discharges at surface, a specific temperature needs to be selected, here termed the
reference temperature. For sub-boiling and non-thermal waters, the first choice for reference
temperature is the measured temperature of the water at the time of sampling. Inevitable
daily variations in the temperature of surface waters may affect the measured temperatures,
but such changes are considered to be relatively small. Also, the temperatures of the waters
may reflect mixing of two or more water components of different temperatures. If the water
sources have significantly different temperatures, the calculated fluid composition of the
mixed water, based on the mixed temperature, will match neither any reservoir water with
this temperature nor any aqueous species activities that may have equilibrated locally with
specific minerals.
It has been suggested that geothermal systems are characterized by anisotropic permeability
where hot water flow is controlled by tectonic fractures. Under this assumption, the water
entering a well or discharging from a spring must be a mixture of many components from
different sources of varying distances as dictated by the three dimensional distribution of the
permeability. Therefore, the analytical data of the fluid samples becomes unreliable for
testing local mineral-solution equilibrium/disequilibrium. The best conditions for assessing
equilibrium are met when temperature remains relatively constant with depth within the
geothermal system. The situation is more complicated for two-phase hot water wells because
the measured temperature at the wellhead does not represent the reservoir temperature. Also,
data from the water and steam samples collected at the wellhead/surface may not easily
reconstruct the chemical composition of the reservoir. Although boiling is commonly
34
assumed to be adiabatic for such calculations, the mechanism may be characterized by an
open system where vapour and gases can separate from the liquid phase. Such degassing is
dealt with in the WATCH program by assigning an arbitrary degassing coefficient for
example.
In the present study, the reference temperatures for all the samples with temperatures greater
than 100 °C were based on calculated geothermometry temperatures. If the quartz
geothermometer yielded T<180 °C, this was the temperature used. If it yielded T>180 °C,
then the chalcedony geothermometer temperature was used. This changeover temperature
has been found to be valid for most active geothermal systems associated with geologically
young volcanic rocks (Stefánsson & Arnórsson, 2000). However, the silica geothermometry
is based on the assumption of equilibrium between solution and chalcedony or quartz, and
proof may be lacking to verify this assumption. Partial re-equilbrization may also have
occurred during cooling in the upflow, causing an underestimation of aquifer temperatures.
The use of geothermometry for estimating the reservoir temperatures of geothermal waters
may seem to be a circular argument. This study avoids this issue by studying the saturation
state of the feldspars at a temperature that corresponds to equilibrium either with chalcedony
or quartz or with measured aquifer temperatures.
In addition to the silica geothermometry, other cation geothermometers based on Na, K, Ca,
and Mg were used to estimate the reservoir temperatures. The geothermometers and their
equations are listed Table 4.3 and their results later compared. Once the reservoir
temperatures were chosen, WATCH was again used to reconstruct reservoir fluid
composition and pH prior to boiling.
Following, aqueous speciation and mineral saturation states were calculated using the
PHREEQC program. These calculations used the reservoir pH from the WATCH program,
as this is based on the measured pH values assigned to the reservoir temperature assuming
conservation of alkalinity.
Alteration minerals observed in cuttings and cores of Mount Meager wells included smectite,
chlorite, illite, saponite, talc, epidote, K-feldspar, actinolite, carbonate, quartz, hematite,
pyrite, and Fe-Ti oxides (Moore et al., 1985). Surface and near-surface deposits include
calcite, siderite, dolomite, quartz, K-feldspar, and pyrite veins. Saturation indices could not
be calculated for Al- and Fe-bearing minerals as these elements were not in included in
geochemical analysis of most fluids. Instead, mineral-fluid reactions of secondary minerals
were balanced, then 𝑙𝑜𝑔𝑄 for each reaction was calculated based on cation activities (𝑎)
calculated by PHREEQC and, for some reactions, reservoir pH or anion concentration. The
input was the database of reservoir composition, pH, and temperature listed in Appendix C.
These reactions and calculations are listed in Table 4.4. Finally, the solubility (𝑙𝑜𝑔𝐾) was
calculated for each reaction and graphed with 𝑙𝑜𝑔𝑄 to assess how closely each mineral
approached equilibrium.
Distribution of geothermal activity
The distribution of major components was mapped to help visualize the distribution of
geothermal activity as well as hydrogeochemical controls on thermal fluid movement. From
the calculated reservoir temperature and composition, averages of CO2, SO4, and Cl content
35
and temperature were calculated for each sample location. The data were input into ArcMap
version 10.5 (Esri, 2016) where sample location coordinates have previously been mapped
(Proenza, 2012). Following, the components were analyzed using the Natural Neighbor
interpolation tool to interpolate values between samples (Sibson, 1981).
36
Table 4.3 Equations for geothermometers used. Concentrations are in mg/kg. T is in °C.
Geothermometer Equation for T Range Source
Quartz −42.2 + 0.28831𝑆𝑖𝑂2 − 3.6686 × 10−4(𝑆𝑖𝑂2)2 + 3.1665× 10−7(𝑆𝑖𝑂2)3 + 77.034𝑙𝑜𝑔𝑆𝑖𝑂2
25-900 Fournier and Potter (1982)
Quartza −53.5 + 0.11236𝑆𝑖𝑂2 − 0.5559 × 10−4(𝑆𝑖𝑂2)2 + 0.1772× 10−7(𝑆𝑖𝑂2)3 + 88.390𝑙𝑜𝑔𝑆𝑖𝑂2
Fournier and Potter (1982)
Chalcedony 1032
4.69 − 𝑙𝑜𝑔𝑆𝑖𝑂2− 273.15
0-250 Fournier (1977)
Na-K 933
0.993 + 𝑙− 273.15
25-250 Arnórsson et al. (1983b)
K-Ca 1930
3.861 + 𝑙𝑜𝑔(𝐾/√𝐶𝑎)− 273.15
Tonani (1980)
K-Mg 4410
14.00 + 𝑙𝑜𝑔(𝐾2/√𝑀𝑔)− 273.15
Giggenbach (1988)
Na-K-Cab 1647
2.24 + 𝑙𝑜𝑔(𝑁𝑎/𝐾) + 𝛽𝑎 (𝑙𝑜𝑔(√𝐶𝑎/𝑁𝑎))− 273.15
4-340 Fournier and Truesdell (1973)
a Silica concentrations in water initially in equilibrium with quartz after adiabatic boiling to 100 °C. bConcentration in mol/kg. 𝛽 = 4/3 for t<100 °C; 1/3 for t>100 °C and for log(√𝐶𝑎/𝑁𝑎)<0.
37
Table 4.4 Balanced reactions used to calculate loqQ.
Balanced Mineral-Fluid Reactions 𝒍𝒐𝒈𝑸
𝑤𝑜𝑙𝑙𝑎𝑠𝑡𝑜𝑛𝑖𝑡𝑒 + 2𝐻+ + 𝐻2𝑂 = 𝐶𝑎2+ + 𝐻4𝑆𝑖𝑂4 𝑙𝑜𝑔(𝑎𝐻2𝑆𝑂4) + 𝑙𝑜𝑔(𝑎𝐶𝑎2+) + 2𝑝𝐻
0.6𝑔𝑟𝑜𝑠𝑠𝑢𝑙𝑎𝑟 + 2𝐻+ = 0.4𝑐𝑙𝑖𝑛𝑜𝑧𝑜𝑒𝑠𝑖𝑡𝑒 + 0.6𝑞𝑢𝑎𝑟𝑡𝑧 + 0.8𝐻2𝑂 + 𝐶𝑎2+ 𝑙𝑜𝑔(𝑎𝐶𝑎2+) + 2𝑝𝐻
1.5𝑝𝑟𝑒ℎ𝑛𝑖𝑡𝑒 + 2𝐻+ = 𝑐𝑙𝑖𝑛𝑜𝑧𝑜𝑒𝑠𝑖𝑡𝑒 + 1.5𝑞𝑢𝑎𝑟𝑡𝑧 + 4𝐻2𝑂 + 𝐶𝑎2+ 𝑙𝑜𝑔(𝑎𝐶𝑎2+) + 2𝑝𝐻
𝐾𝐹𝑒𝑙𝑑𝑠𝑝𝑎𝑟 + 𝑁𝑎+ = 𝑎𝑙𝑏𝑖𝑡𝑒 + 𝐾+ 𝑙𝑜𝑔(𝑎𝑁𝑎+) − 𝑙𝑜𝑔(𝑎𝐾+)
0.8𝑚𝑢𝑠𝑐𝑜𝑣𝑖𝑡𝑒 + 0.2𝑐𝑙𝑖𝑛𝑜𝑐ℎ𝑙𝑜𝑟𝑖𝑡𝑒 + 5.4𝑞𝑢𝑎𝑟𝑡𝑧 + 2𝐾+ = 2.8𝐾𝐹𝑒𝑙𝑑𝑠𝑝𝑎𝑟 + 1.6𝐻2𝑂 𝑙𝑜𝑔(𝑎𝑀𝑔2+) + 2𝑙𝑜𝑔(𝑎𝐾+)
𝑐𝑎𝑙𝑐𝑖𝑡𝑒 = 𝐶𝑎2+ + 𝐶𝑂32−
𝑙𝑜𝑔(𝑎𝐶𝑎2+) + 𝐶𝑂3−
39
5 Chemical characteristics of samples
The measured temperatures, pH values, and major element concentrations of the water
samples considered here are listed in Appendix A. Measured temperatures of cold springs,
hot springs, and shallow wells ranged from 0-9 °C, 29-39 °C, and 25-69 °C, respectively,
and pH values ranged from 7.3-8.3, 5.9-7.2, and 6.1-8.1, respectively. The pH of these waters
were sampled both on site and in a lab; both sampling techniques yielded similar pH values
within each sample location. All waters sampled from deep wells had alkaline pH values of
8-9, taken at 19-25 °C, and temperatures at bottom hole depths (2300 to 3500 m) of around
215-250 °C.
The Piper Plot in Figure 5.1 illustrates the major chemical features of geothermal waters
from springs and wells in the study area. For the cold springs, along with shallow wells M2
and M7, major cations are Ca2+ and Na+ with small amounts of Mg2+. The major anion is
HCO3- with a trend-line towards increasing SO4
- content, which may be attributed to small
amounts of SO4- remaining in the gas phase. These waters are likely calcium bicarbonate
springs formed by interaction of condensed CO2-rich gas with groundwater and perhaps a
small amount of mixing and are therefore considered peripheral waters.
The Meager Creek Hot Springs, Placid Hot Springs, and well EMR-1, which all lie on the
western edge of the N-S running Meager Creek, classify as sodium alkali chloride and
sodium chloride waters. The dominant cation is Na+, and the waters are variable in Cl- and
CO32- + HCO3
- content, indicating either boiling or mixing of cold bicarbonate water with
Cl--rich reservoir water. The No Good Warm Springs, which lie on the north edge of the E-
W running section of Meager Creek, are chemically similar but classify as sodium
chloride/sodium bicarbonate waters, suggesting a mixing component. The dominant cation
is Na+ but trends towards Ca2+ which also suggests mixing, perhaps with the calcium
bicarbonate cold springs. Overall, these springs are alkali chloride waters and likely
represent mature waters with a component of mixing and/or boiling.
All deep wells are classified as sodium chloride waters with Na+ as the dominant cation.
Anion content, however, varies between wells. MC-1, MC-2, and MC-8 waters are neutral
to slightly alkaline with Cl- as the dominant anion. MC-1 waters trend towards higher
SO42- and HCO3- content. These wells are alkali-chloride waters and represent mature,
unmixed waters.
Waters from MC-3 are high in Cl- but trend toward increasing SO42- content, indicative of a
sulfur input. Waters from the shallow wells M1-74D and M12-80D are similar in
composition. They may classify as acid sulphate-chloride waters which are typical for acid
sulphate primary fluids, where the sulfur is volcanic in origin. However, because the sulfur
source is unknown, MC-3 waters could also be the same alkali chloride waters as MC-1,
MC-2, and MC-3 with a sulfur input.
40
MC-6 waters consist of near-equal proportions of SO42-, Cl-, and HCO3
-. A slight trendline
showing variable Cl- and SO42- content may be indicative of mixing. MC-6 therefore
represents mature waters within the geothermal system.
Figure 5.1 Piper plot of all sampled waters.
41
6 Discussion
The primary purpose of this study was to understand the controls on water chemistry and the
effects of mixing and water-rock interaction at the Mount Meager field, including estimation
of geothermal reservoir temperatures and distribution of the geothermal activity within the
area using the various chemical signatures.
Conservative elements B and Cl were used to trace water sources and mixing of various
waters in geothermal systems as well as progressive water-rock interaction. In meteoric
source water, the concentrations of B and Cl are usually low, and upon water-rock interaction
and mixing with for example seawater, the elemental concentrations and relative ratios
changes. These changes can, in turn, be used to quantify the various sources of the two
elements, including the origin of the water and mixing ratios between water types (Arnórsson
& Andrésdóttir, 1995).
Reservoir temperatures of geothermal fluids are commonly estimated using gas, solute,
and/or isotopic geothermometers. Solute geothermometers are either univarient or ion ratios.
Univarient geothermometers, such as quartz and chalcedony, are based on a single element
concentration and may be subject to secondary changes upon boiling, fluid mixing, and
condensation. Ratio chemical geothermometers like Na-K overcome this challenge by using
element ratios that are affected to the same degree by these secondary processes like boiling.
They are, however, limited by equilibrium and rate conditions. Geothermometry is based on
the assumption that chemical equilibrium is attained between the reservoir fluids and
secondary geothermal minerals. Such equilibrium may not have been attained in some cases,
and re-equilibration with other minerals upon fluid ascent to surface may also occur. It is,
therefore, important to assess if fluid-mineral equilibrium is truly attained within the
geothermal system. The geothermal reservoir temperatures determined from
geothermometery calculations may be used to assess the reservoir fluid composition.
Moreover, for waters of various origin, for example a mixture of surface and geothermal
reservoir water, such calculations have limited significance.
Fluid origin and mixing using boron and
chloride systematics
The relationships between B and Cl concentration, and the Cl/B molal ratio with chloride
concentration are shown in Figure 6.1. Chloride and B concentrations ranged from 100 to
3300 ppm and 0.3 to 28 ppm, respectively. Hot spring waters contained the lowest Cl and B
content (100-675 ppm and 1-3.3 ppm), followed by deep well waters MC-3 and MC-6, MC-
1 and MC-2, MC-8 (250-3030 ppm and 1.6-20.7 ppm), and finally shallow wells with the
highest concentrations (2640-3300 ppm, 22-28.2 ppm). The latter were possibly
anomalously high due to sampling error. Non-thermal springs do not include B data but
contain the lowest Cl content (0.3-1.2 ppm).
42
The mixing trends between non-thermal waters and geothermal waters are difficult to assess
based on the chloride and boron relations. First, data on B concentration are often missing,
especially for the non-thermal waters. Second, the trends when data are available for both
elements showed a cluster of Cl values between 500-3000 ppm. In all cases, a positive linear
relationship between Cl and B concentration was observed, and most samples had similar
Cl/B molal ratios. They grouped from 30-55, apart from MC-6 waters, which showed a
linear increase from 25 to 37. The Cl and B concentrations of the waters were far too high,
and Cl/B ratios far too low, to consider seawater or meteoric water (precipitation) as the
dominant source of Cl and B. In contrast, the Cl and B systematics suggest the water to be
of meteoric origin with Cl and B concentrations similar to what can be expected in the region,
followed by leaching of Cl and B from the primary rocks and minerals. Given the geological
complexity of the area, it is highly unlikely that all the reservoir fluids have encountered the
same host rock composition and mineralogy in all cases, and the waters reflected more
closely the Cl/B ratio of basalts rather than andesite. The reason for this is unclear. Also, the
Cl and B content reflects high rock to water ratio (ξ) corresponding to >1 kg of rock dissolved
per liter of water. Such high values may suggest an additional source of Cl and B than only
dissolution of primary rocks, for example direct magmatic degassing (e.g., White, 1970;
Bégué et al., 2015). Given the linear Cl and B systematics, a magmatic gas source of similar
origin would be more likely rather than multiple magmatic sources. Characterizing and
quantifying the magmatic component using only these relations is difficult if not impossible
due to similar chemical signals as upon rock leaching (Bégué et al., 2015). However, the
generally elevated Cl and B concentrations of Mount Meager thermal waters may be
indicative of magma degassing associated with slab subduction (Symonds, 1992; Sanchez,
1993; Arnórsson, 2000; Bégué et al., 2015. Guðmundsson, 2015; McCaig et al., 2018; Wang
& Xiao, 2018). Such elemental addition been observed from stable water isotope systematics
of subduction related geothermal systems (Giggenbach, 1992).
Re-sampling fluids to include B concentrations, as well as gathering B and Cl data on
precipitation and rock composition, would be beneficial to continue the conservative element
analysis of the thermal waters.
43
Figure 6.1 The relationship between (A) B and Cl and (B) Cl/B molal ratio and Cl for the
thermal waters. Precipitation content is plotted along with average compositions of
andesite and basalt. Progressive rock leaching (ξ) from 0.01 to 1 is also graphed
44
Reservoir temperature and fluid composition
Reservoir temperatures are commonly estimated using gas, chemical, and isotopic
geothermometers which utilize equations or models based on temperature-dependent fluid-
rock equilibria. Here, various geothermometry temperatures were calculated (see Table 4.3).
The results are given in Appendix B and compared in Figure 6.2. Negative values are
considered unrealistic, so only positive values were plotted. The ranges of each
geothermometer for cold springs, hot springs, shallow wells, and deep wells are summarized
in Table 6.1. For all temperatures, the chalcedony geothermometer yielded results that
closely followed those of quartz, calculating slightly lower temperatures. For quartz
geothermometer temperatures of Tquartz<100-150 °C, the Na-K and K-Ca cation
geothermometers calculated highly scattered and unusually high temperatures, while the K-
Mg and Na-K-Ca geothermometers linearly increased with increasing Tquartz. For
temperatures Tquartz>100-150 °C, the cation geothermometer temperatures did not increase
with increasing Tquartz. The K-Ca geothermometer calculated the lowest temperatures,
followed by K-Mg, Na-K, and finally Na-K-Ca geothermometer yielding the highest
temperatures.
The Na-K and K-Ca geothermometry data are likely scattered at Tquartz <100-150 °C because
ratio chemical geothermometers are limited by equilibrium which may not be attained in low
temperature and non-thermal waters. Fluid mixing may also contribute to the observed
trends.
At temperatures around 150-250 °C, the solubility of quartz controls the concentration of
dissolved silica, and equilibrium between water and quartz is closely approached at around
180°C (Fournier & Rowe, 1977). At lower temperatures, chalcedony appears to control
dissolved silica concentration, while equilibrium is closely approached between water and
chalcedony at about 100 °C (Fournier, 1977). Therefore, the quartz geothermometer and
chalcedony geothermometer were taken as reservoir temperature if the quartz
geothermometer yielded temperatures above 180 °C and between 100 to 180 °C,
respectively. For samples with measured temperature of less than 100°C, the measured
temperature was used as reservoir temperature. These reservoir temperatures are reported in
Appendix B and range from 4.5 to 9.0 °C, 29.5 to 56.0 °C, 10.1 to 68.5 °C, and 101.6 to
282.8 °C for cold springs, hot springs, shallow wells, and deep wells, respectively.
Table 6.1 Temperatures ranges for all geothermometers for each well and hot spring type.
Geothermometer Cold Springs Hot Springs Shallow Wells Deep Wells
Quartz 19.1-65 105.6-172.5 49.6-172.3 129.3-282.8
Chalcedony -9.6-32.7 75.6-149.7 17.6-149.5 101.6-268
Na/K 134.7-214.4 201.1-284.2 96.8-321.8 141.3-252.4
K/Ca 270.9-359.6 134.1-181.3 139.4-269.7 81.0-182.6
K/Mg 1.1-55.3 97.8-123.3 60.8-128.0 105.9-242.9
Na-K-Ca -43.2-25.8 99.8-162.1 34.7-162.3 154.2-246.4
45
Figure 6.2 Comparison of different geothermometers.
Using the selected reservoir temperatures, reservoir fluid composition was calculated using
the WATCH program. Here, we used the results both to construct reservoir fluid composition
of boiled waters and to assess the effects of boiling on fluid composition. The WATCH
program reads the chemical analysis of waters sampled at the surface and computes chemical
composition of downhole fluids. WATCH ran a boiling hot springs model using equilibrium
degassing and boiling temperature of 100 °C. The model cannot calculate results for samples
with reservoir temperatures of T<100 °C (cold springs, hot springs, EMR-1, M1-74D, M2-
75D, M7-79D, and M12-80D), so they were considered non-boiled waters and their sampled
compositions were taken as reservoir compositions. For wells with reservoir temperatures of
T>100 °C (MC-1, MC-2, MC-3, MC-6, and MC-8), results from the boiling hot spring model
are taken as reservoir composition. The compositions are reported in Appendix C.
The concentration ranges of these samples are given in Table 6.2. For MC-1 and MC-2, the
concentration range of each element was large, especially for CO2 and SO4. MC-3 samples
had a more moderate range in element concentration, while MC-6 and MC-8 had low
concentration variations within each element. For non-boiled waters from cold springs, hot
springs, and shallow wells, reservoir compositions are the same as previously described.
46
Table 6.2 Range of concentrations for reservoir compositions of samples that degassed.
MC-1 MC-2 MC-3 MC-6 MC-8
B 6.3 – 13.2 2.7 – 49.6 1.4 – 8.5 3.6 – 8.1 14.7 – 15.8
SiO2 86.7 – 342.6 124.1 – 367.9 211.3 – 361.4 97.9 – 192.3 408.0 – 462.1
Na 615.8 –
1238.8
347.9 –
5010.4 255.3 – 982.8
724.4 –
1201.6
1267.0 –
1316.8
K 47.8 – 107.1 24.4 – 429.5 23.8 – 68.7 40.9 – 91.4 200.3 – 212.4
Mg 0.2 – 96.7 0.5 – 13.6 0.7 – 2.5 0.2 – 5.7 0.02 – 0.2
Ca 2.8 – 408.6 29.1 – 725.3 10.3– 96.4 48.8 – 62.6 33.8 – 47.7
F 0.1 – 2.6 0.7 – 6.9 0.6 – 2.1 – 1.7
Cl 823.0 –
1898.7
504.5 –
7921.2
220.1 –
1206.4 302.2 – 686.9
2164.0 –
2306.2
CO2 282.7 –
43692.5
243.2 –
11277.4
170.8 –
3240.7
5110.0 –
23789.7
3582.4 –
6279.0
SO4 71.4 – 946.8
117.4 –
1336.1 283.0 – 473.8 356.0 – 421.3 65.9 – 71.0
To assess the how boiling affects water composition from the reservoir to surface, fluid
composition was compared between the boiling hot springs (degassing) model and the
sampled compositions. For all deep wells, major element component concentration (SiO2,
Mg, Cl, B, Na, K, Ca) increased only slightly compared to the sampled compositions. CO2
and SO4 content change is shown in Figure 6.3. Comparing results between the degassing
model and sampled composition suggests that CO2 content changes for some sample
locations when degassing is considered, while SO4 content does not. Samples from MC-6
have experienced moderate to significant CO2 degassing between 100-150 °C. MC-1 has
undergone CO2 degassing at around 190 °C. Some waters from MC-1 and MC-2 were
sampled with high SO4 content; this concentration did not alter significantly with the boiling
hot springs model. These samples also did not alter in CO2 concentration when degassing
was considered, indicating that the surface waters represent reservoir waters in terms of CO2
and SO4 gas content. This suggests that a source such as magma contributes to the high in
these waters. Non-boiled waters from M1-74D and M12-80D were even higher in SO4
content.
47
Figure 6.3 CO2 and SO4 composition of all waters from sampling (blue) and for wells
using reservoir composition calculated from WATCH.
48
6.2.1 Fluid-mineral interaction
The activities of major aqueous species were used to study the saturation state of geothermal
waters. Past studies have suggested that the composition of geothermal waters is controlled
by equilibrium between minerals and solution for major components of the system except
chloride (Ellis, 1970; Michard, 1991; Arnórsson & Andrésdóttir, 1995). For example,
equilibrium is closely approached between water and microcline, a form of K-feldspar, and
low-albite for temperatures above 200 °C (Browne, 1978; Stefánsson & Arnórsson, 2000).
It has been suggested that this equilibrium, based on the reaction low-albite + K+ =
microcline + Na+, controls the Na+/K+ activity ratio in high temperature waters (Giggenbach,
1981; Arnórsson et al., 1983a). Similarly, the equilibrium between the solution and
wollastonite and H2SO4, grossular, clinozoesite, and quartz, prehnite, clinozoesite and
quartz, muscovite, clinochlorite, quartz, and K-feldspar, and calcite controls the activities of
H2SO4 and Ca2+, Ca2+, Ca2+, Mg2+ and K+, and Ca2+, respectively, based on the reactions
listed in Table 4.4. The solubility constants of each reaction are based on the assessment of
thermodynamic data of the minerals, as well as thermodynamic properties of liquid water.
For this study, variations of major cation activities with reservoir temperature were studied
and compared to their respective solubility curves. The select cations are based on alteration
minerals observed in the system, including epidote (as clinozoesite), calcite, chlorite (as
clinochlorite), K-feldspar, and quartz together with wollastonite, garnet (grossular) and
prehnite that have not been unambiguously reported within the geothermal system. As Fe
and Al concentrations were rarely reported in the dataset of the fluid samples, mineral buffer
reactions were constructed to study mineral-fluid equilibria together with some single
mineral- solute reactions. The following chemical reactions were considered:
A. wo + 2H+ + H2O = Ca2+ + H4SiO4
B. 0.6gro + 2H+ = 0.4czo + 0.6qtz + 0.8H2O + Ca2+
C. 1.5pre + 2H+ = czo + 1.5qtz + 4H2O + Ca2+
D. K-feld + Na+ = alb + K+
E. 0.8mus + 0.2chl + 5.4qtz + 2K+ = 2.8K-feld + 1.6H2O + Mg2+
F. cc = Ca2+ + CO32-
where wo = wollastonite, gro = grossular, czo = clinozoesite, qtz = quartz, pre = prehnite,
K-feld = K-feldspar, alb = albite, mus = muscovite, chl = clinochlore and cc = calcite.
49
The reaction quotients (𝑄) based on the aqueous speciation calculations are compared with
solubility curves (𝑙𝑜𝑔𝐾) for the reactions as a function of reservoir temperature in Figure
6.4. Figure 6.4A,B,C all show very similar trends with 𝑙𝑜𝑔𝑄 values lower than the
corresponding 𝑙𝑜𝑔𝐾 values, but following the solubility curve as temperature increases with
some minor offsets. Figure 6.4D shows minerals approaching saturation and reaching
equilibrium at reservoir temperatures around 200-250 °C. Minerals in Figure 6.4E follow
the saturation curve and reach 𝑙𝑜𝑔𝑄 values greater than 𝑙𝑜𝑔𝐾 values above approximately
150 °C. In Figure 6.4F, it appears that equilibrium is reached with the minerals and solution
for all reservoir temperatures, with some minor offsets.
These data suggest that activities of H2SO4 and Ca2+, Ca2+, and Mg2+ and K+ are likely
controlled by equilibrium between the solution and secondary minerals observed in the
geothermal systems. The slight discrepancies observed in Figure 6.4 may be attributed to
several factors. Many of the secondary minerals involved are solid-solutions which affected
the exact value of the mineral buffer equilibrium values. Further, the calculations of the
reaction quotients rely on the aqueous speciation to be accurate. The current dataset does
not allow such assessment and calculations in most cases and are in turn dependent on
assumptions. Complete samples of liquid and vapour phases from T>100 °C samples were
not available, resulting in reconstruction of the vapour phase during modeling. The pH of
the reservoir fluids was further constructed from such calculations with the measured pH
sometimes not available. These all led to uncertainties in calculating reservoir fluid aqueous
species distribution as well as reaction quotients. In fact, inspection of calcite saturation
revealed systematic undersaturation suggesting some problems related to, for example,
reconstruction of pH, aqueous species activities, and modeling steam and CO2 loss upon
boiling. Many of these problems related to the limitations of the available data. Indeed, in
cases of reactions where such effects were minor, like involving K-feldspar and albite and
the Na+/K+ ion ratio, a very close approach to equilibrium at T>175 °C was observed (Fig.
6.4D). Also, inspection of the figure reveals water mixing at reservoir temperatures below
around 175 °C.
Overall, the cation activities indicate that equilibrium is observed between secondary
minerals and solution at high temperatures, and that there is likely mixing of colder waters
with the thermal fluids. The observed trends are in accordance with other geothermal waters
globally, especially the close approach between calcite and solution (i.e. Giggenbach, 1981;
Arnórsson et al., 1983a, Stefánsson & Arnórsson, 2000; Arnórsson, 1978; Arnórsson, 1989).
Future fluid analyses that includes Fe and Al content will be imperative for confirming which
secondary minerals control water composition, as the balanced mineral reactions use
assumptions about end-member compositions of solid solutions. These assumptions may
affect the calculations, as well as the database used for calculated 𝑙𝑜𝑔𝐾 of each reaction.
Future studies extending from this research may consider addressing these assumptions and
calculations to better understand the mineral-solution equilibria.
50
Figure 6.4 Activities of major cations as a function of temperautre. The solid line shows
logK for each reaction.
51
Distribution of geothermal activity
To further understand the geothermal activity and its distribution within the MMVC, key
variables were mapped. The distribution of these parameters may indicate hydrogeological
and geochemical controls and distribution on the system. The mean and standard deviation
of Cl, SO4, CO2, and temperature for each location are listed in Table 6.3. These averages
were used to create the distribution maps in Figure 6.5. Highest temperatures are found at
deep well MC-8 and extend to MC-1 and MC-2. There is also a temperature anomaly at MC-
3. Temperature decreases with distance away from these wells and is lowest at shallow wells
M2-75D and M7-79D, as well as both cold springs. Cl distribution is high around the
temperature peak at MC-8, MC-1, and MC-2, and also increases around shallow well M1-
74D, and further increases towards the south at M12-80D. This southerly-trending anomaly
is correlated with the elevated SO4 concentration of the waters. There is also a slight SO4
content elevation around MC-6. CO2 content peaks around deep well MC-6 and decreases
with distance from MC-6.
The overall data suggest a significant source of hot, Cl- and CO2-rich thermal waters around
deep wells MC-1, MC-2, MC-6, and MC-8, and possibly MC-3, although more data is
required to confirm the latter. The Carbonate Fault or the No Good Discontinuity to the east
of MC-3 may be controlling cold water supply to the CaCO3 Cold Spring and to M7. The
east-west running Meager Creek Fault Zone may structurally control the Cl- and SO4-rich
waters presenting at M1-74D and M12-80D to the south, with the source of Cl and SO4
possibly related to rock composition or deep magma degassing. The latter is, however, not
correlated with elevated CO2 concentration as would be expected.
Aside from the deep wells, distance between sample locations is large, creating greater
uncertainty in the respective contour lines. Anomalies and patterns in these areas are
therefore more difficult to constrain and more data points are required to optimize the
distribution maps. Many of the shallow wells are situated between these locations but are
missing complete data sets and therefore could not be considered for analysis. Future
research may involve re-sampling of fluids from these wells to decrease the size of the
contour lines and better understand the subsurface reservoir.
52
Table 6.3 Averages and standard devations of reservoir Cl, CO2, SO4 and temperature for
sample locations. Concentrations are in ppm; temperatures are in °C.
Location Cl CO2 SO4 Temp
Mean StDev Mean StDev Mean StDev Mean
Meager Creek Hot
Springs 492.2 148.6 458.3 94.9 115.2 45.2 48.6
No Good Hot Springs 258.2 109.7 357.0 79.3 66 25.8 31.3
Placid Cold Springs 674.0 398.0 2.0 45.1
Boundary Cold Springs 66.3 2.0 5.0
CaCO3 Cold Springs 0.6 0.5 316.0 39.2 33.3 17.3 7.0
Problem Cold Springs 0.8 594.0 36.1 9.3
EMR-1 541.8 63.5 525.0 99.3 178.0 4.7 59.9
M1-74D 2670.0 30.0 1136.5 136.5 2285.0 85.0 54.2
M2-75D 0.6 233.0 22.6 10.1
M7-79D 40.0 200.0 47.0 25.0
M12-80D 3300.0 499.0 2800.0 -
MC-1 1626.7 181.7 2768.0 4490.1 122.8 78.4 213.6
MC-2 1941.8 2172.4 2403.3 3035.3 283.0 357.0 211.6
MC-3 792.5 294.7 1727.9 988.7 346.2 51.4 198.6
MC-6 587.9 198.2 10799.8 6749.1 391.6 24.5 128.3
MC-8 2216.9 63.5 5288.9 1211.8 68.0 2.2 275.5
For simplification, M1-74D, M2-75D, M7-79D, and M12-80D are shown on figures as M1,
M2, M7, and M12, respectively.
53
54
Figure 6.5 Distribution of key variables Cl, CO2, SO4, and temperature.
55
7 Conclusions
For this study, geochemistry of thermal fluids from the southern reservoir at Mount Meager
was analyzed to delineate fluid origin, reservoir temperature and composition, degree of
mixing and boiling, and saturation state of the waters.
Conservative element analysis used chloride and boron content of the waters to understand
degree of water-rock interaction and mixing and to identify the sources for the fluids. High
Cl and B concentrations of 100 to 3300 ppm and 0.3 to 28 ppm, respectively, as well as high
Cl/B molal ratios of 25 to 55, indicated that a single magmatic source is likely contributing
to fluid composition.
Several geothermometers were compared, and the quartz and chalcedony geothermometry
results were taken as reservoir temperature when the quartz geothermometery yielded
temperatures of Tquartz>180 °C and 100 °C<Tquartz<180 °C, respectively. Measured
temperature was taken as the reservoir temperature for low-temperature samples. Reservoir
temperatures ranged from 4.5 to 9.0 °C, 29.5 to 56.0 °C, 10.1 to 68.5 °C, and 101.6 to 282.8
°C for cold springs, hot springs, shallow wells, and deep wells, respectively. Calculated
reservoir fluid compositions indicate that wells MC-1 and MC-6 experienced significant CO2
degassing during fluid ascent, while high SO4 content of wells to the south of the Meager
Creek Fault Zone can be traced down to the reservoir. Saturation states of the waters
indicated that the Mount Meager south reservoir is of a typical geothermal system where the
thermal waters are controlled by equilibrium between the solution and observed secondary
minerals at high temperatures. The results also suggested a component of colder water
mixing with the thermal waters.
Hot springs and wells on the eastern and northern sides of the reservoir, which are of low
temperature and low CO2, likely define the boundaries of peripheral waters. Wells to the
southeast contained anomalously high Cl and SO4, suggesting a magmatic input of these
components that may be controlled by the east-west running Meager Creek Fault Zone.
There is a significant source hot, Cl- and CO2-rich thermal waters supplying deep wells MC-
1, MC-2, MC-6 and MC-8, and possibly MC-3. These NaCl waters likely define the high
temperature, central location of the geothermal reservoir. Overall, the deep wells seem to
have drilled into the high-temperature geothermal reservoir at Mount Meager.
Additional research on several geological aspects can help to further understand the system.
In terms of fluid chemistry, a more complete chemical analysis of the fluids that includes
more major elements, especially Al and Fe, will improve the raw data set. Mineral-solution
equilibrium systematics can also be further studied to understand the fluid system. To
improve conservative element analysis, B and Cl content of the host rock and precipitation
is required. Structurally, the MMVC is not well understood and can benefit greatly from
more in-depth fault and fracture mapping.
57
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65
Appendix A
Final database after data filtering, and input for WATCH. T is temperature in °C. Element concentrations are in ppm.
Sample Name T pH SiO2 B Na K Ca Mg Fe F Cl HCO3 SO4
Meager Creek (Souther 1976) 55 164.0 450.0 47.0 81.0 25.0 675.0 468.0 110
Meager Creek (N.S-B.G 1974) 59 7.20 164 2.00 450 47 81 25.0 0.00 675 468.0 110
Meager Creek (Hammerstrom
1977) 31 6.50 56 165 23.7 92 15.4 0.45 133 503.0 25
Meager Creek (Hammerstrom
1977) 30 6.80 54 248 27 83.5 17.1 0.50 295 260.0 50
Meager Creek (Hammerstrom
1977) 49 6.40 80.5 347 44 92 24.8 0.00 428 450.0 65
Meager Creek (Hammerstrom
1977) 56 6.05 92 377 46.2 94 34.1 0.15 466 458.0 170
Meager Creek (Hammerstrom
1977) 57 6.15 96 410 52 105 40.5 0.30 500 686.0 180
Meager Creek (Hammerstrom
1977) 50 6.60 102 390 48.5 92 31.0 0.00 500 595.0 145
Meager Creek (Grasby 2000) 47 7.20 172 419 44.6 77.5 24.7 0.05 543 445.0 125
Meager Creek (vent #19; Clark et
al 1980) 50 6.24 142 440 50 78 24.5 605 437.0 130
Meager Creek main vent (Table 1,
GT7, N.S-B.G 1975) 58 6.6 150 330 54 51 15 600 504 190
Meager Creek main vent (NSBG,
1981; NSBG 1980) 50 6.54 162 439 45.5 81.9 26.2 0.12 528 464 122
66
Meager Creek main vent (NSBG,
1981; Shenker, 1980) 57 6.6 170 3.3 400 43 80 24 0.30 560 350 110
Meager Creek main vent (NSBG,
1981; Shenker, 1980) 48 6.5 180 440 46 86 24 0.30 600 400 120
Upper Meager Creek (Spring 79D)
(NSBG 1975) 33 6.7 108 150 32 40 275 387 76
Placid Hot Springs Vent 2 (NSBG
1981; Clark et al 1980) 45 5.89 138 433 53.5 114 27.6 0.35 674 398 174
No Good Warm Spring #1 (NSBG
1981; Hammerstrom and Brown,
1977)
30 6.8 54 248 27 83.5 17.1 295 260 50
No Good Warm Spring #1 (NSBG
1981; Shenker, 1980) 35 6.4 120 320 32 88 16 470 310 110
No Good Warm Spring #2 (NSBG
1981; NSBG 1975) 33 6.7 108 150 32 40 7.6 275 387 76
No Good Warm Spring #2 (NSBG
1981; Hammerstrom and Brown,
1977)
31 6.5 56 165 23.7 92 15.4 133 503 25
No Good Warm Spring #2 (NSBG
1981; Clark et al, 1980) 30 6.82 101 175 22.4 75.6 13.7 196 382 69
No Good Warm Spring #2 (NSBG
1981; Clark et al, 1980) 30 6.8 110 160 22 82 14 180 300 66
Boundary Cold Springs (NSBG
1981; Clark et al 1980) 5 8.31 6 4.84 0.54 12.2 5.42 0 0 66.3 2.02
CaCO3 Cold Springs (NSBG
1981; NSBG 1975) 9 7.96 21 3.2 0.16 95 9.6 0.5 278 44
CaCO3 Cold Springs (NSBG
1981; Shenker 1980) 7 7.3 10 3 2 120 15 1.2 300 47
CaCO3 Cold Springs (NSBG
1981; Clark et al 1980) 6 7.62 8.9 3.2 1.75 98.6 12.5 0 370 8.95
67
Problem Cold Spring #1 (Clark et
al 1980) 9 7.65 10.9 11.9 5 106 44.9 0.8 594 36.1
EMR-1 (NSBG 1981;
Hammerstrom and Brown, 1977) 56 6.05 92 377 46.2 97 34.1 0.15 466 458 170
EMR-1 (NSBG 1981;
Hammerstrom and Brown, 1977) 57 6.15 96 410 52 105 40.5 0.3 500 686 180
EMR-1 (NSBG 1981; Clark et al,
1980) 58 6.06 155 424 48.4 107 36.2 0.14 571 526 182
EMR-1 (NSBG 1981; Shenker,
1980) 69 6.6 180 440 46 120 38 0.3 630 430 180
M1-74D (NSBG 1981; Clark et al,
1980) 52 6.23 104 22 2390 98.1 223 90.3 0.16 2640 1273 2370
M1-74D (NSBG 1981; Clark et al,
1980) 56 6.6 110 2400 79 400 94 0.9 2700 1000 2200
M2-75D (NSBG 1981; Clark et al
1980) 10 7.7 15.5 23 6.93 32.9 18 0.1 0.56 233 22.6
M7-79D (NSBG 1981) 25 8.09 14 28 4.2 72 8 0.48 0.18 40 200 47
M12-80D (NSBG 1981) 6.53 110 28.2 2800 130 440 360 3300 499 2800
MC-1 MM-32 6.7 87 9.2 820 48 410 97 0.15 1060 990 950
MC-1 MM-35 7 140 7.2 700 69 3 65 0.4 870 966 400
MC-1 MM-36 7.7 21 -1 24 1.6 15 3.5 -0.1 0.55 50 -5
MC-1 17/03/1982 8.4 430 7.9 1050 74 26 0.2 2.9 1440 74 210
MC-1 07/07/1982 8.3 320 11 1130 84 36 0.2 2.1 1660 80 160
MC-1 09/07/1982 6.3 350 10.8 1100 80 31 0.4 2.2 1640 53 150
MC-1 22/07/1982am1 8.6 300 9.7 1160 82 43 0.2 2.2 1770 64 160
MC-1 22/07/1982pm2 8.5 300 8.6 980 74 42 0.5 2 1520 54 140
MC-1 22/07/1982web1 7.9 280 9.3 1100 80 44 0.2 2.2 1680 79 150
MC-1 22/07/1982web2 8.2 340 9.2 1110 82 46 0.3 2.2 1690 71 150
MC-1 17/08/1982 1000 8.3 363 11.8 1100 88 39 0.6 2.1 1780 52 140
MC-1 10/09/1982 0900 8.3 370 9.8 870 74 134 1.4 1.4 1360 245 210
68
MC-1 12/09/1982 0400 8.1 324 14.6 1400 102 60 0.3 2.3 2130 119 220
MC-1 13/09/1982 1300 7.5 280 14.8 1350 105 91 0.6 2.2 2190 32 150
MC-1 14/09/1982 1030 8.5 171 14 1320 106 73 0.6 2.6 1940 70 140
MC-1 14/09/1982 1100 8.3 168 13.6 1310 114 62 0.4 2.8 1980 50 140
MC-1 14/09/1982 1200 8.2 159 14.1 1330 106 54 0.4 2.7 2000 50 150
MC-1 14/09/1982 1100 8 185 12.1 1140 104 55 0.4 2.6 1790 50 120
MC-1 14/09/1982 1130 8.2 165 13.6 1220 104 53 0.4 2.7 1910 48 130
MC-1 25/09/1982 8.4 373 13.1 1210 94 36 0.6 2.2 1930 46 150
MC-1 27/09/1982 8.5 376 12.4 1210 95 37 0.8 2 1940 41 140
MC-1 01/10/1982 8.3 374 13.4 1260 99 37 1 2.3 1990 57 140
MC-1 09/10/1982 8.3 217 13 1250 98 37 1 2.3 1930 50 130
MC-1 18/10/1982 1200 8.4 390 13 1290 108 38 0.8 2.1 2070 46 130
MC-1 23/10/1982 1200 8.3 370 12.8 1260 98 40 0.8 2.1 1990 52 120
MC-1 24/10/1982 1200 8.2 390 13.2 1320 100 37 1 2 2030 69 130
MC-1 25/10/1982 1200 8.2 400 13.8 1320 101 37 1 2.1 2040 68 130
MC-1 28/10/1982 2400 8.7 340 7.6 740 59 33 0.8 1.8 1090 51 170
MC-1 29/10/1982 0800 8.2 370 11.6 1130 92 47 1 1.9 1720 52 160
MC-1 29/10/1982 2400 8.7 400 14.5 1440 114 82 1.5 2.3 2210 54 190
MC-1 30/10/1982 0800 8.6 290 13.7 1310 101 74 4.6 2 2020 51 170
MC-1 30/10/1982 2400 8.4 330 15 1420 106 64 20 2.6 2210 63 190
MC-1 31/10/1982 0830 8.1 330 15.4 1480 126 65 23 2.8 2270 61 170
MC-1 07/11/1982 1200 8.4 360 12.6 1190 97 41 1.2 1.9 1940 43 150
MC-1 09/11/1982 1200 8.2 340 11.9 1170 95 37 1.2 1.8 1870 46 130
MC-1 11/11/1982 0715 8.3 370 12.8 1210 100 37 1.2 1.9 1990 45 140
MC-1 11/11/1982 0945 8.3 390 13.4 1220 100 37 1.3 2 2030 48 130
MC-1 11/11/1982 0945 8.3 360 12.2 1180 96 36 1.2 1.9 1940 45 130
MC-1 15/11/1982 1200 8.1 220 8.1 750 61 36 1.7 1.3 1210 46 86
69
MC-1 20/11/1982 1100 8.3 360 13.1 1270 100 37 1.2 2 1980 45 130
MC-1 23/11/1982 1100 8.3 360 12.8 1270 100 36 1.3 2 1970 44 130
MC-1 23/11/1982 1400 7 260 10.3 940 75 27 0.9 1.5 1490 54 96.8
MC-1 28/11/1982am 8.3 370 13.3 1280 93 36 1.3 2 1990 39 140
MC-1 01/12/1982pm 8.3 390 13.3 1280 93 37.1 1.4 2 1990 40 130
MC-1 06/12/1982 1400 8.2 370 13.5 1270 93 36.5 1.4 2 1990 41 140
MC-1 09/12/1982 1400 8.3 380 13.8 1260 92 36.5 1.4 2 2000 37 140
MC-1 12/12/1982 1000 8.3 380 13.4 1260 93 36 1.4 2 2080 39 140
MC-1 15/12/1982 0900 8.4 380 13.8 1270 92 35.5 1.4 2 1990 38 140
MC-1 19/12/1982 0900 8.3 370 13.6 1280 93 36 1.4 2 1990 38 140
MC-1 23/12/1982 0900 8.3 390 14 1310 110 36 1.6 2.1 2000 44 130
MC-1 26/12/1982 1200 8.3 370 13.4 1290 110 37 1.5 2.1 1990 44 130
MC-1 29/12/1982 1200 8.3 370 13.6 1290 113 46 1.4 2.1 2010 44 140
MC-1 02/01/1983 1600 8.7 380 13.6 1290 110 37 1.4 2.1 1980 66 140
MC-1 05/01/1983 1300 8.2 380 14 1270 112 36 1.4 1.9 1980 45 130
MC-1 09/01/1983 0900 8.2 370 13.5 1270 118 36 1.4 1.9 1970 45 120
MC-1 13/01/1983 1500 8.2 390 14 1280 112 36 1.3 2 1990 45 120
MC-1 16/01/1983 1500 8.2 380 13.8 1280 118 36 1.3 2 1990 45 120
MC-1 20/01/1983 1300 8.3 360 13.9 1280 120 38 1.3 1.9 1960 45 120
MC-1 30/01/1983 0900 8.4 350 15 1380 125 45 1.2 2.1 2100 47 130
MC-1 02/02/1983 1200 8.6 390 15.1 1520 117 58 0.7 2.5 2280 8.6 130
MC-1 06/02/1983 1730 8.5 350 13.6 1360 106 52 0.4 2.2 1930 38 140
MC-1 09/02/1983 1500 7.1 360 12.7 1180 97 55 3.8 1.9 1870 126 120
MC-1 13/02/1983 2030 8.6 390 15.1 1420 110 45 0.2 2.3 2220 40 140
MC-1 19/02/1983 1200 8.4 370 14 1320 106 39 1.1 2.2 2090 42 150
MC-1 24/02/1983 0900 8.4 380 14.1 1330 107 38 1.3 2.2 2100 35 140
MC-1 27/02/1983 0900 8.4 380 14 1290 109 38 1.4 2.1 2080 35 160
70
MC-1 02/03/1983 1330 8.4 380 14.4 1300 117 39 1.5 2.8 2060 33 130
MC-1 06/03/1983 0900 8.3 370 14.3 1330 116 39 1.5 2.7 2040 36 130
MC-1 09/03/1983 0900 8.4 370 14 1320 114 39 1.5 2.7 2030 34 130
MC-1 13/03/1983 0900 8.4 380 13.9 1320 109 40 1.4 2.8 2060 35 130
MC-1 16/03/1983 0900 8.4 380 13.6 1310 111 38 1.5 2.7 2050 34 130
MC-1 20/03/1983 0900 8.4 380 14.5 1280 110 39 1.5 2.7 2040 34 130
MC-1 23/03/1983 0900 8.4 380 13.8 1290 114 39 1.5 2.7 2040 34 130
MC-1 27/03/1983 0900 8.4 370 14.6 1310 113 40 1.5 2.7 2030 34 130
MC-1 30/03/1983 8.5 380 15 1290 110 38.6 1.3 2 2060 40 140
MC-1 03/04/1983 8.5 410 16 1420 120 41.9 0.5 2.2 2230 42 140
MC-1 06/04/1983 8.4 410 15 1320 110 38.8 0.4 2.2 2130 42 130
MC-1 10/04/1983 8.4 310 14 1320 110 37.6 1.4 2 2060 43 140
MC-1 14/04/1983 8.4 370 14 1310 120 36.2 1.5 2 2030 43 140
MC-1 18/04/1983 8.4 380 13 1280 110 36.2 1.6 2 2040 43 140
MC-1 21/04/1983 8.4 380 14 1360 120 37.9 1.6 1.9 2020 44 140
MC-1 24/04/1983 8.4 390 14 1260 110 36 1.6 1.9 2010 43 140
MC-1 27/04/1983 8.4 390 14 1310 110 36.5 1.6 1.9 2020 42 140
MC-1 01/05/1983 8.4 380 14 1280 110 36.1 1.6 1.9 2010 43 140
MC-1 04/05/1983 8.4 380 15 1270 110 34.2 1.6 1.9 2010 40 130
MC-1 08/05/1983 8.4 350 15 1290 110 36 1.6 1.9 2000 43 140
MC-1 12/05/1983 0930 8.4 370 14 1280 100 35 1.5 2.2 2000 43 140
MC-1 05/06/1983 0900 8.3 380 14 1350 110 34 1.5 2.2 2000 42 130
MC-1 09/06/1983 0900 8.4 370 14 1250 100 34 1.5 2.2 2000 44 120
MC-1 12/06/1983 0900 8.4 370 14 1240 100 34 1.5 2.2 2000 41 150
MC-1 16/06/1983 8.3 370 14 1240 100 34 1.5 2.2 2010 44 150
MC-1 19/06/1983 8.4 360 14 1240 100 34 1.5 2.2 2010 44 150
MC-1 22/06/1983 8.4 400 14 1270 110 33 1.7 2.1 2010 43 150
71
MC-1 26/06/1983 8.3 350 14 1270 110 33 1.6 2.1 2010 42 160
MC-1 29/06/1983 8.4 350 14 1270 110 33 1.6 2.1 2000 41 150
MC-1 03/07/1983 8.4 340 14 1260 110 32 1.6 2 1990 41 150
MC-1 04/09/1983 8.2 280 15 1360 110 53 0.7 2.4 2130 69 150
MC-1 11/09/1983 8.3 340 15 1370 110 49 1 2.5 2110 61 120
MC-1 18/09/1983 8.3 360 15 1370 120 50 1 2.6 2130 58 130
MC-1 09/10/1983 8.4 340 14 1320 120 36 1.4 2.5 2040 39 130
MC-1 16/10/1983 8.4 330 14 1300 120 36 1.5 2.4 2030 38 130
MC-1 23/10/1983 8.3 340 14 1260 110 35 1.5 2.5 2030 38 140
MC-1 05/12/1983 0900 8.5 220 14 1330 120 34 1.4 2 1430 29 88
MC-1 05/12/1983 8.3 270 11 1040 90 26 1.1 1.6 2030 36 140
MC-1 11/12/1983 0900 8.5 280 12 1098 92 27 1.1 1.7 1330 28 83
MC-1 11/12/1983 8.3 320 12 1180 100 29 1.3 1.8 2020 36 150
MC-1 18/12/1983 0900 8.4 280 12 1050 89 27 1.1 1.7 2010 43 130
MC-1 18/12/1983 8.3 260 10 980 86 25 1.1 1.5 1550 29 120
MC-1 25/12/1983 0900 8.4 340 15 1300 110 31 1.4 2.1 2020 42 130
MC-1 25/12/1983 8.3 360 13 1290 110 33 1.4 2 2030 38 140
MC-1 01/01/1984 0900 8.4 340 14 1290 110 32 1.3 2.1 2010 42 130
MC-1 01/01/1984 8.4 350 13 1290 110 32 1.4 2 2030 35 140
MC-1 12/01/1984 0900 8.4 350 14 1300 110 32 1.4 2.1 2010 42 130
MC-1 15/01/1984 8.3 350 14 1310 110 33 1.4 2 2030 36 140
MC-1 22/01/1984 0900 8.4 350 14 1310 110 31 1.3 2.1 2020 41 130
MC-1 22/01/1984 8.4 350 14 1310 110 33 1.3 2 2020 36 140
MC-1 29/01/1984 0900 8.4 360 15 1290 110 31 1.3 2.1 2010 42 130
MC-1 29/01/1984 8.2 310 13 1230 91 46 1 2 2010 36 140
MC-1 15/07/1984 8.6 360 15 1370 120 37 0.8 2 2140 21 130
MC-1 25/07/1984 8.6 360 15 1370 120 35 0.8 2.2 2160 18 130
72
MC-1 31/07/1984 8.4 360 15 1360 120 38 0.8 2.1 2150 29 130
MC-1 09/08/1984 8.4 360 15 1380 120 38 0.8 2.2 2150 28 130
MC-1 15/08/1984 8.4 370 15 1370 120 38 0.9 2.3 2140 26 120
MC-1 23/08/1984 8.4 370 15 1370 120 38 0.9 2.3 2150 36 120
MC-1 31/08/1984 8.4 360 16 1370 130 37 0.9 2.3 2150 36 120
MC-1 06/09/1984 8.4 370 15 1360 120 38 0.9 2.3 2140 36 120
MC-1 13/09/1984 8.6 370 15 1350 120 37 0.8 2.3 2140 26 120
MC-1 20/09/1984 8.4 370 15 1360 120 38 0.8 2.3 2140 34 120
MC-1 28/09/1984 8.4 370 15 1380 130 37 0.8 2.3 2140 35 120
MC-1 04/10/1984 8.4 360 14 1350 130 37 0.9 2.3 2140 35 120
MC-2 03/06/1982 8.5 240 5.6 740 72 33 4.3 0.8 990 106 200
MC-2 22/10/1982 0800 8.8 260 3.1 400 28 50 1.5 0.8 580 30 180
MC-2 23/10/1982 1000 8.6 430 6.8 700 58 58 1.7 1.5 1070 42 160
MC-2 24/10/1982 1400 2.4 440 9.4 820 77 55 1.8 1.5 1340 11 160
MC-2 25/10/1982 0600 8.7 470 10.5 950 93 49 0.6 1.6 1490 32 150
MC-2 13/11/1982 1000 8.3 270 12.7 1160 92 130 6.6 1.5 1820 41 180
MC-2 13/11/1982 1400 9.1 320 19.9 2010 180 140 6.3 2.6 3010 31 420
MC-2 13/11/1982 1600 8.5 410 12.8 1110 92 100 9.1 1.8 1760 42 160
MC-2 13/11/1982 1800 8.5 430 12.9 1190 104 180 17 2.2 1900 25 190
MC-2 13/11/1982 1900 7 130 52 5250 450 760 2.2 7.2 8300 58 1400
MC-3 16/10/1982 1900 9.1 340 6 770 52 32 0.8 1.7 850 101 420
MC-3 20/10/1982 1600 9.6 450 10.4 1180 78 106 2.7 2.6 1360 39 590
MC-3 21/10/1982 1000 8.5 260 9.6 1130 79 26 2.9 1.2 470 114 400
MC-3 25/10/1982 2000 8.3 240 1.6 290 27 50 1.9 0.7 250 68 370
MC-3 26/10/1982 0400 8.4 290 3.3 450 37 26 1.8 1 450 87 390
MC-3 26/10/1982 2000 9.3 380 6.1 810 61 118 2.3 1.8 900 91 550
MC-3 27/10/1982 0900 8.7 320 5.1 630 51 28 2.4 1.2 750 111 390
73
MC-3 28/10/1982 1000 9.1 290 7.1 800 59 12 0.9 1.2 960 61 390
MC-3 02/11/1982 1400 8.8 320 6.7 770 57 20 1.6 1.3 950 101 360
MC-3 02/11/1982 2200 8.6 330 7.3 800 58 25 2.2 1.4 960 112 390
MC-3 09/11/1982 1200 8.8 340 8.9 960 70 19 1.4 1.3 1330 107 340
MC-3 09/11/1982 2000 9 280 9.3 970 66 29 1.9 1.7 1270 90 390
MC-3 11/11/1982 1436 8.9 300 9.9 970 71 13 0.8 1.4 1280 120 350
MC-3 11/11/1982 1834 9 240 9.7 1010 71 35 1.3 1.9 1370 71 410
MC-6 166.51 7.71 161 3.86 779 43.95 67.33 4.07 325 382 453
MC-6 177.76 7.84 215 4.92 868 58.78 68.74 6.39 448 352 398
MC-6 190.97 8.07 122 8.09 1290 93.86 55.5 1.46 848 382 442
MC-6 193.68 133 8.89 1322 100.5 57 0.2 849 305 422
MC-6 195.59 8.76 8.9 1200 94.6 47.9 1080
MC-6 190.38 7.88 105 6.58 943 74.65 52.37 0.23 737 290
MC-8 (Thermochem Air Lift
Analysis, 2008) 7.95 630 20.1 1760 273 46.1 0.027 2.36 2950 43.1 91.6
MC-8 (Thermochem Air Lift
Analysis, 2008) 8.02 619 20.1 1720 279 47.4 0.03 2.35 2960 46.9 89.4
MC-8 (Thermochem Air Lift
Analysis, 2008) 7.37 536 20.7 1730 279 62.6 0.212 2.21 3030 11.8 93.3
75
Appendix B
Geothermometry calculations. Temperatures are in °C.
Sample Name Measured Quartz Chalcedony Na/K K/Ca K/Mg Na-K-Ca Reservoir
Meager Creek (Souther 1976) 55.0 165.1 141.4 205.6 148.4 115.2 145.6 55.0
Meager Creek (N.S-B.G 1974) 59.0 164.3 140.5 205.6 148.4 115.2 145.6 59.0
Meager Creek (Hammerstrom
1977) 01 31.4 107.4 77.5 241.5 180.6 99.2 100.1 31.4
Meager Creek (Hammerstrom
1977) 03 30.0 105.6 75.6 210.9 172.4 102.0 112.7 30.0
Meager Creek (Hammerstrom
1977) 05 48.5 125.4 97.3 227.3 153.6 113.3 134.9 48.5
Meager Creek (Hammerstrom
1977) 06 (GSC1) 56.0 132.6 105.3 222.9 152.0 112.4 137.6 56.0
Meager Creek (Hammerstrom
1977) 17 (GSC1) 56.5 134.9 107.8 226.5 149.5 114.7 140.9 56.5
Meager Creek (Hammerstrom
1977) 18 50.0 138.0 111.3 224.5 149.6 114.6 141.0 50.0
Meager Creek (Grasby 2000) 47.0 167.3 143.9 207.5 149.6 113.8 143.4 47.0
Meager Creek (vent #19; Clark et
al 1980) 49.8 157.7 133.1 214.6 145.1 117.2 149.3 49.8
Meager Creek main vent (Table 1.
GT7. N.S-B.G 1975) 57.5 160.7 136.4 253.9 134.1 123.3 162.1 57.5
Meager Creek main vent (NSBG.
1981; NSBG 1980) 50.1 165.6 142.0 204.7 149.9 113.9 143.4 50.1
Meager Creek main vent (NSBG.
1981; Shenker. 1980) 57.0 168.6 145.3 208.7 151.7 112.9 140.1 57.0
76
Meager Creek main vent (NSBG.
1981; Shenker. 1980) 47.5 172.5 149.7 205.6 150.4 114.9 142.4 47.5
Upper Meager Creek (Spring
79D) (NSBG 1975) 33.0 141.2 114.7 284.2 149.6 133.0 33.0
Placid Hot Springs Vent 2 (NSBG
1981; Clark et al 1980) 45.1 156.1 131.4 223.5 150.0 118.4 140.5 45.1
No Good Warm Spring #1 (NSBG
1981; Hammerstrom and Brown.
1977)
30.0 105.6 75.6 210.9 172.4 102.0 112.7 30.0
No Good Warm Spring #1 (NSBG
1981; Shenker. 1980) 34.5 147.5 121.8 201.1 166.1 107.3 121.5 34.5
No Good Warm Spring #2 (NSBG
1981; NSBG 1975) 33.0 141.2 114.7 284.2 149.6 112.7 133.0 33.0
No Good Warm Spring #2 (NSBG
1981; Hammerstrom and Brown.
1977)
31.4 107.4 77.5 241.5 180.6 99.2 100.1 31.4
No Good Warm Spring #2 (NSBG
1981; Clark et al. 1980) 29.5 137.3 110.4 228.4 178.6 98.4 103.6 29.5
No Good Warm Spring #2 (NSBG
1981; Clark et al. 1980) 29.5 142.1 115.8 236.3 181.3 97.8 99.8 29.5
Boundary Cold Springs (NSBG
1981; Clark et al 1980) 4.5 19.1 -9.6 214.4 359.6 22.8 2.2 4.5
CaCO3 Cold Springs (NSBG
1981; NSBG 1975) 8.5 65.0 32.7 134.7 1.1 -43.2 8.5
CaCO3 Cold Springs (NSBG
1981; Shenker 1980) 7.0 37.6 6.5 345.0 42.2 -5.1 7.0
CaCO3 Cold Springs (NSBG
1981; Clark et al 1980) 5.6 33.4 2.7 348.0 40.5 -4.7 5.6
Problem Cold Spring #1 (Clark et
al 1980) 9.0 40.7 9.3 270.9 55.3 25.8 9.0
EMR-1 (NSBG 1981;
Hammerstrom and Brown. 1977) 56.0 132.6 105.3 222.9 152.7 112.4 136.7 56.0
EMR-1 (NSBG 1981;
Hammerstrom and Brown. 1977) 56.5 134.9 107.8 226.5 149.5 114.7 140.9 56.5
77
EMR-1 (NSBG 1981; Clark et al.
1980) 58.4 163.3 139.4 214.8 152.8 113.4 137.6 58.4
EMR-1 (NSBG 1981; Shenker.
1980) 68.5 172.3 149.5 205.2 157.3 111.5 132.6 68.5
M1-74D (NSBG 1981; Clark et al.
1980) 52.3 139.2 112.6 111.6 139.4 128.0 159.2 52.3
M1-74D (NSBG 1981; Clark et al.
1980) 56.0 142.0 115.7 96.8 159.8 120.9 144.1 56.0
M2-75D (NSBG 1981; Clark et al
1980) 10.1 53.7 21.5 321.8 216.3 67.5 60.6 10.1
M7-79D (NSBG 1981) 49.6 17.6 246.4 269.7 60.8 34.7
M12-80D (NSBG 1981) 142.1 115.8 121.9 141.6 125.9 162.3
MC-1 MM-32 129.3 101.6 144.7 182.6 105.9 154.2 101.6
MC-1 MM-35 155.1 130.2 197.4 81.0 118.3 226.1 130.2
MC-1 17/03/1982 234.6 220.6 161.5 114.9 165.2 190.2 234.6
MC-1 07/07/1982 209.3 191.6 168.7 115.2 171.6 192.1 209.3
MC-1 09/07/1982 221.8 206.1 166.1 114.6 162.7 191.6 221.8
MC-1 22/07/1982am1 202.7 184.1 164.0 118.9 171.0 188.1 202.7
MC-1 22/07/1982pm2 204.2 185.8 170.7 122.1 158.5 188.9 204.2
MC-1 22/07/1982web1 200.3 181.3 166.9 120.0 170.4 188.6 200.3
MC-1 22/07/1982web2 215.1 198.3 168.0 120.4 166.5 188.9 215.1
MC-1 17/08/1982 1000 220.8 204.8 175.9 115.4 162.3 194.8 220.8
MC-1 10/09/1982 0900 219.9 203.9 181.5 144.3 148.3 182.2 219.9
MC-1 12/09/1982 0400 209.9 192.4 166.0 117.3 175.2 190.1 209.9
MC-1 13/09/1982 1300 202.5 183.9 173.5 123.2 170.3 189.4 202.5
MC-1 14/09/1982 1030 162.7 138.7 177.6 117.8 172.7 193.6 138.7
MC-1 14/09/1982 1100 163.6 139.7 185.8 112.5 179.7 199.7 139.7
MC-1 14/09/1982 1200 160.6 136.3 176.7 112.5 177.0 196.3 136.3
MC-1 14/09/1982 1100 171.4 148.5 190.8 113.8 175.7 200.8 148.5
78
MC-1 14/09/1982 1130 163.1 139.1 183.7 112.9 176.1 198.7 139.1
MC-1 25/09/1982 222.6 206.9 172.8 111.9 164.6 195.7 222.6
MC-1 27/09/1982 222.8 207.2 174.0 112.0 162.3 196.0 222.8
MC-1 01/10/1982 222.9 207.3 174.1 110.6 161.8 196.8 222.9
MC-1 09/10/1982 180.8 159.1 175.0 109.5 163.9 197.4 180.8
MC-1 18/10/1982 1200 226.5 211.3 180.5 108.3 167.0 200.7 226.5
MC-1 23/10/1982 1200 222.2 206.5 173.3 112.2 163.5 195.5 222.2
MC-1 24/10/1982 1200 226.5 211.4 170.4 110.4 161.9 195.5 226.5
MC-1 25/10/1982 1200 228.8 214.0 171.3 110.2 162.2 196.1 228.8
MC-1 28/10/1982 2400 213.3 196.3 175.3 126.2 145.7 188.8 213.3
MC-1 29/10/1982 0800 222.9 207.2 177.4 117.1 159.1 194.5 222.9
MC-1 29/10/1982 2400 225.8 210.5 174.3 119.5 162.9 192.1 225.8
MC-1 30/10/1982 0800 200.1 181.1 172.7 121.0 149.9 190.3 200.1
MC-1 30/10/1982 2400 211.8 194.6 169.0 117.2 138.4 191.1 211.8
MC-1 31/10/1982 0830 213.3 196.3 182.4 111.6 143.0 199.4 213.3
MC-1 07/11/1982 1200 219.7 203.7 177.8 112.9 159.5 196.9 219.7
MC-1 09/11/1982 1200 215.8 199.1 177.7 111.7 159.0 197.5 215.8
MC-1 11/11/1982 0715 222.5 206.8 179.2 110.3 160.5 199.0 222.5
MC-1 11/11/1982 0945 227.0 212.0 178.4 110.4 159.5 198.6 227.0
MC-1 11/11/1982 0945 220.2 204.2 177.8 111.1 159.2 197.9 220.2
MC-1 15/11/1982 1200 183.4 162.0 179.2 125.3 142.1 190.0 183.4
MC-1 20/11/1982 1100 220.1 204.0 174.5 110.2 160.7 197.2 220.1
MC-1 23/11/1982 1100 220.1 204.1 174.5 109.7 159.9 197.4 220.1
MC-1 23/11/1982 1400 197.0 177.5 176.8 113.6 154.3 195.7 197.0
MC-1 28/11/1982am 222.7 207.0 166.3 112.2 157.1 192.9 222.7
MC-1 01/12/1982pm 227.3 212.3 166.3 112.9 156.2 192.5 227.3
MC-1 06/12/1982 1400 223.1 207.5 167.0 112.5 156.4 193.1 223.1
79
MC-1 09/12/1982 1400 225.1 209.8 166.7 112.9 155.9 192.7 225.1
MC-1 12/12/1982 1000 225.0 209.7 167.8 112.3 156.3 193.4 225.0
MC-1 15/12/1982 0900 224.5 209.1 165.9 112.4 155.9 192.6 224.5
MC-1 19/12/1982 0900 222.7 207.1 166.3 112.2 156.4 192.9 222.7
MC-1 23/12/1982 0900 227.1 212.0 180.8 106.8 161.1 201.7 227.1
MC-1 26/12/1982 1200 222.5 206.8 182.5 107.1 162.0 202.1 222.5
MC-1 29/12/1982 1200 222.5 206.9 185.2 109.8 163.6 201.6 222.5
MC-1 02/01/1983 1600 220.6 204.6 182.6 107.2 162.5 202.1 220.6
MC-1 05/01/1983 1300 225.2 209.9 185.9 106.2 163.2 204.0 225.2
MC-1 09/01/1983 0900 222.9 207.3 191.6 104.4 165.3 207.2 222.9
MC-1 13/01/1983 1500 227.5 212.5 185.2 106.3 163.7 203.7 227.5
MC-1 16/01/1983 1500 225.2 209.9 190.7 104.5 165.8 206.9 225.2
MC-1 20/01/1983 1300 220.1 204.0 192.6 104.7 166.8 207.5 220.1
MC-1 30/01/1983 0900 216.8 200.3 189.0 106.0 169.2 205.2 216.8
MC-1 02/02/1983 1200 226.1 210.9 172.1 112.7 171.3 194.8 226.1
MC-1 06/02/1983 1730 216.6 200.0 173.5 113.8 173.5 194.7 216.6
MC-1 09/02/1983 1500 221.1 205.2 179.0 117.9 149.2 194.4 221.1
MC-1 13/02/1983 2030 224.7 209.3 172.6 110.5 181.3 196.3 224.7
MC-1 19/02/1983 1200 221.9 206.1 176.2 109.2 163.5 198.5 221.9
MC-1 24/02/1983 0900 224.5 209.1 176.4 108.6 162.2 199.0 224.5
MC-1 27/02/1983 0900 224.6 209.2 181.1 108.0 162.2 201.3 224.6
MC-1 02/03/1983 1330 224.7 209.3 188.1 106.1 164.2 204.9 224.7
MC-1 06/03/1983 0900 222.8 207.1 184.8 106.3 164.0 203.6 222.8
MC-1 09/03/1983 0900 222.3 206.6 183.9 106.8 163.3 202.8 222.3
MC-1 13/03/1983 0900 224.6 209.2 179.2 108.8 162.2 199.9 224.6
MC-1 16/03/1983 0900 224.6 209.3 181.8 107.4 162.2 201.7 224.6
MC-1 20/03/1983 0900 224.6 209.3 183.3 108.1 161.8 201.9 224.6
80
MC-1 23/03/1983 0900 224.7 209.3 186.2 106.9 163.2 203.7 224.7
MC-1 27/03/1983 0900 222.3 206.5 183.7 107.5 163.0 202.3 222.3
MC-1 30/03/1983 223.5 208.0 182.4 107.9 163.2 201.7 223.5
MC-1 03/04/1983 230.1 215.5 181.3 106.6 175.3 202.1 230.1
MC-1 06/04/1983 231.1 216.5 179.9 108.2 174.1 200.5 231.1
MC-1 10/04/1983 207.1 189.1 180.5 106.9 163.5 201.4 207.1
MC-1 14/04/1983 221.9 206.1 189.8 104.0 165.2 207.0 221.9
MC-1 18/04/1983 224.3 208.9 183.1 106.9 161.2 202.6 224.3
MC-1 21/04/1983 224.1 208.7 185.9 104.8 164.5 204.9 224.1
MC-1 24/04/1983 226.6 211.5 184.7 106.8 161.1 203.2 226.6
MC-1 27/04/1983 226.6 211.4 180.7 107.1 161.1 201.5 226.6
MC-1 01/05/1983 224.2 208.8 183.1 106.8 161.2 202.6 224.2
MC-1 04/05/1983 224.3 208.9 184.1 105.9 161.3 203.5 224.3
MC-1 08/05/1983 217.0 200.6 182.6 106.5 161.7 202.5 217.0
MC-1 12/05/1983 0930 221.9 206.1 173.5 109.3 158.5 197.4 221.9
MC-1 05/06/1983 0900 224.8 209.4 177.8 105.8 161.8 201.1 224.8
MC-1 09/06/1983 0900 221.9 206.1 176.2 108.9 158.5 198.6 221.9
MC-1 12/06/1983 0900 222.0 206.2 176.6 108.9 158.5 198.9 222.0
MC-1 16/06/1983 222.5 206.8 176.5 108.9 158.5 198.9 222.5
MC-1 19/06/1983 219.5 203.4 176.7 108.8 158.6 198.9 219.5
MC-1 22/06/1983 228.8 214.0 183.6 105.5 160.4 203.7 228.8
MC-1 26/06/1983 217.7 201.3 183.9 105.1 161.7 204.0 217.7
MC-1 29/06/1983 217.2 200.7 184.0 105.1 161.7 204.0 217.2
MC-1 03/07/1983 214.7 197.9 184.9 104.5 161.8 204.7 214.7
MC-1 04/09/1983 199.4 180.3 177.5 112.3 170.6 197.0 199.4
MC-1 11/09/1983 214.6 197.7 176.8 111.5 166.2 197.1 214.6
MC-1 18/09/1983 219.5 203.4 185.4 109.1 169.3 202.0 219.5
81
MC-1 09/10/1983 214.8 198.0 189.4 103.6 166.3 206.9 214.8
MC-1 16/10/1983 212.4 195.2 191.1 103.6 165.8 207.5 212.4
MC-1 23/10/1983 215.5 198.8 185.0 106.0 162.4 203.8 215.5
MC-1 05/12/1983 0900 180.8 159.0 189.8 101.6 168.3 207.8 180.8
MC-1 05/12/1983 197.5 178.2 184.7 107.1 158.9 202.8 197.5
MC-1 11/12/1983 0900 199.3 180.1 181.9 107.0 159.6 201.5 199.3
MC-1 11/12/1983 210.7 193.3 182.0 105.9 160.5 202.7 210.7
MC-1 18/12/1983 0900 199.4 180.3 182.6 108.1 158.3 201.3 199.4
MC-1 18/12/1983 195.1 175.4 186.4 107.8 157.4 202.9 195.1
MC-1 25/12/1983 0900 214.6 197.7 182.0 104.0 163.1 203.7 214.6
MC-1 25/12/1983 220.3 204.3 182.4 105.2 162.8 203.3 220.3
MC-1 01/01/1984 0900 214.7 197.8 182.8 104.5 163.7 203.7 214.7
MC-1 01/01/1984 217.5 201.0 182.5 104.6 162.9 203.7 217.5
MC-1 12/01/1984 0900 217.1 200.6 181.9 104.6 162.9 203.4 217.1
MC-1 15/01/1984 218.0 201.6 180.9 105.1 162.9 202.7 218.0
MC-1 22/01/1984 0900 217.1 200.6 181.1 104.1 163.6 203.4 217.1
MC-1 22/01/1984 217.3 200.9 181.0 105.1 163.6 202.7 217.3
MC-1 29/01/1984 0900 219.4 203.3 182.6 104.2 163.5 203.9 219.4
MC-1 29/01/1984 208.6 190.9 168.5 116.6 159.6 191.1 208.6
MC-1 15/07/1984 218.5 202.2 185.5 104.2 171.4 205.0 218.5
MC-1 25/07/1984 218.6 202.3 185.4 103.4 171.4 205.5 218.6
MC-1 31/07/1984 220.0 203.9 186.1 104.7 171.4 205.0 220.0
MC-1 09/08/1984 220.0 204.0 184.6 104.7 171.4 204.4 220.0
MC-1 15/08/1984 222.5 206.8 185.4 104.8 170.1 204.7 222.5
MC-1 23/08/1984 222.0 206.3 185.4 104.8 170.1 204.7 222.0
MC-1 31/08/1984 219.6 203.5 193.9 101.7 173.4 209.9 219.6
MC-1 06/09/1984 222.0 206.3 186.2 104.8 170.1 205.0 222.0
82
MC-1 13/09/1984 220.7 204.7 187.1 104.3 171.3 205.5 220.7
MC-1 20/09/1984 222.1 206.4 186.2 104.8 171.3 205.0 222.1
MC-1 28/09/1984 222.1 206.3 193.0 101.8 174.4 209.5 222.1
MC-1 04/10/1984 219.8 203.7 195.4 101.7 173.4 210.5 219.8
MC-2 03/06/1982 186.5 165.6 196.5 118.2 139.6 200.8 186.5
MC-2 22/10/1982 0800 193.5 173.5 162.9 162.7 117.6 167.4 193.5
MC-2 23/10/1982 1000 236.0 222.0 178.7 138.1 137.6 184.2 236.0
MC-2 24/10/1982 1400 244.2 231.1 194.4 126.7 146.6 194.7 244.2
MC-2 25/10/1982 0600 243.4 230.2 196.0 118.2 163.0 201.0 243.4
MC-2 13/11/1982 1000 197.7 178.4 175.5 134.3 143.8 184.4 197.7
MC-2 13/11/1982 1400 194.4 174.5 186.5 112.4 167.8 200.9 194.4
MC-2 13/11/1982 1600 231.6 217.2 179.4 130.8 139.2 187.8 231.6
MC-2 13/11/1982 1800 237.4 223.6 184.6 137.4 137.9 186.5 237.4
MC-2 13/11/1982 1900 151.0 125.6 179.6 108.0 222.6 201.8 151.0
MC-3 16/10/1982 1900 205.7 187.5 155.9 130.2 141.4 180.6 205.7
MC-3 20/10/1982 1600 210.8 193.4 153.8 138.1 143.9 176.0 210.8
MC-3 21/10/1982 1000 191.1 170.8 160.3 111.2 145.8 192.0 191.1
MC-3 25/10/1982 2000 189.2 168.6 188.5 164.0 115.1 176.9 189.2
MC-3 26/10/1982 0400 202.0 183.2 174.5 138.6 124.4 183.7 202.0
MC-3 26/10/1982 2000 211.2 193.9 165.5 149.5 137.4 175.5 211.2
MC-3 27/10/1982 0900 206.9 188.9 173.4 128.3 131.9 188.2 206.9
MC-3 28/10/1982 1000 193.3 173.3 165.5 108.4 145.4 195.7 193.3
MC-3 02/11/1982 1400 205.5 187.2 165.3 118.4 138.9 190.1 205.5
MC-3 02/11/1982 2200 209.5 191.9 162.6 121.8 136.7 187.5 209.5
MC-3 09/11/1982 1200 209.4 191.8 164.3 110.8 146.8 193.8 209.4
MC-3 09/11/1982 2000 190.8 170.5 158.3 119.4 142.9 186.4 190.8
MC-3 11/11/1982 1436 197.0 177.5 165.3 103.8 152.7 198.1 197.0
83
MC-3 11/11/1982 1834 179.4 157.5 161.8 119.7 149.4 187.5 157.5
MC-6 2230 166.5 160.7 136.4 141.3 84.4 242.8 244.0 136.4
MC-6 40 177.8 178.6 156.6 157.9 84.1 242.9 246.4 156.6
MC-6 515 191.0 141.3 114.8 165.3 87.7 219.6 243.2 114.8
MC-6 745 193.7 151.3 126.0 169.4 148.8 125.4 165.8 126.0
MC-6 190.4 134.9 107.8 177.3 138.6 130.1 176.7 107.8
MC-8 (Thermochem Air Lift
Analysis. 2008) 13851-2 282.8 268.0 247.6 117.3 159.5 190.1 282.8
MC-8 (Thermochem Air Lift
Analysis. 2008) 13851-3 279.6 265.4 252.4 115.6 181.1 192.7 279.6
MC-8 (Thermochem Air Lift
Analysis. 2008) 13851-4 264.2 251.5 251.2 124.0 168.7 189.6 264.2
85
Appendix C
Reservoir fluid compositions calculated using WATCH. Temperatures are in °C; element concentrations are in ppm.
Sample Name B SiO2 Na K Mg Ca F Cl Fe CO2 SO4
Meager Creek (Souther 1976) 164 450 47 25 81 675 468 110
Meager Creek (N.S-B.G 1974) 2 164 450 47 25 81 0 675 468 110
Meager Creek (Hammerstrom
1977) 01 56 165 23.7 15.4 92 133 0.45 503 25
Meager Creek (Hammerstrom
1977) 03 54 248 27 17.1 83.5 295 0.5 260 50
Meager Creek (Hammerstrom
1977) 05 80.5 347 44 24.8 92 428 0 450 65
Meager Creek (Hammerstrom
1977) 06 (GSC1) 92 377 46.2 34.1 94 466 0.15 458 170
Meager Creek (Hammerstrom
1977) 17 (GSC1) 96 410 52 40.5 105 500 0.3 686 180
Meager Creek (Hammerstrom
1977) 18 102 390 48.5 31 92 500 0 595 145
Meager Creek (Grasby 2000) 172 419 44.6 24.7 77.5 543 0.05 445 125
Meager Creek (vent #19; Clark et
al 1980) 142 440 50 24.5 78 605 437 130
Meager Creek main vent (Table 1,
GT7, N.S-B.G 1975) 150 330 54 15 51 600 504 190
Meager Creek main vent (NSBG,
1981; NSBG 1980) 162 439 45.5 26.2 81.9 528 0.12 464 122
Meager Creek main vent (NSBG,
1981; Shenker, 1980) 3.3 170 400 43 24 80 0.3 560 350 110
86
Meager Creek main vent (NSBG,
1981; Shenker, 1980) 180 440 46 24 86 0.3 600 400 120
Upper Meager Creek (Spring
79D) (NSBG 1975) 108 150 32 0 40 275 387 76
Placid Hot Springs Vent 2 (NSBG
1981; Clark et al 1980) 138 433 53.5 27.6 114 674 0.35 398 174
No Good Warm Spring #1 (NSBG
1981; Hammerstrom and Brown,
1977)
54 248 27 17.1 83.5 295 260 50
No Good Warm Spring #1 (NSBG
1981; Shenker, 1980) 120 320 32 16 88 470 310 110
No Good Warm Spring #2 (NSBG
1981; NSBG 1975) 108 150 32 7.6 40 275 387 76
No Good Warm Spring #2 (NSBG
1981; Hammerstrom and Brown,
1977)
56 165 23.7 15.4 92 133 503 25
No Good Warm Spring #2 (NSBG
1981; Clark et al, 1980) 101 175 22.4 13.7 75.6 196 382 69
No Good Warm Spring #2 (NSBG
1981; Clark et al, 1980) 110 160 22 14 82 180 300 66
Boundary Cold Springs (NSBG
1981; Clark et al 1980) 6 4.84 0.54 5.42 12.2 0 0 66.3 2.02
CaCO3 Cold Springs (NSBG
1981; NSBG 1975) 21 3.2 0.16 9.6 95 0.5 278 44
CaCO3 Cold Springs (NSBG
1981; Shenker 1980) 10 3 2 15 120 1.2 300 47
CaCO3 Cold Springs (NSBG
1981; Clark et al 1980) 8.9 3.2 1.75 12.5 98.6 0 370 8.95
Problem Cold Spring #1 (Clark et
al 1980) 10.9 11.9 5 44.9 106 0.8 594 36.1
EMR-1 (NSBG 1981;
Hammerstrom and Brown, 1977) 92 377 46.2 34.1 97 466 0.15 458 170
EMR-1 (NSBG 1981;
Hammerstrom and Brown, 1977) 96 410 52 40.5 105 500 0.3 686 180
87
EMR-1 (NSBG 1981; Clark et al,
1980) 155 424 48.4 36.2 107 571 0.14 526 182
EMR-1 (NSBG 1981; Shenker,
1980) 180 440 46 38 120 0.3 630 0 430 180
M1-74D (NSBG 1981; Clark et al,
1980) 22 104 2390 98.1 90.3 223 2640 0.16 1273 2370
M1-74D (NSBG 1981; Clark et al,
1980) 110 2400 79 94 400 0.9 2700 0 1000 2200
M2-75D (NSBG 1981; Clark et al
1980) 15.5 23 6.93 18 32.9 0.56 0.1 233 22.6
M7-79D (NSBG 1981) 14 28 4.2 8 72 0.18 40 0.48 200 47
M12-80D (NSBG 1981) 28.2 110 2800 130 360 440 3300 499 2800
MC-1 MM-32 9.2 86.7 817.2 47.8 96.7 408.6 0.1 1056.4 5485.9 946.8
MC-1 MM-35 6.8 132.5 662.2 65.3 61.5 2.8 0.4 823.1 43692.5 378.4
MC-1 17/03/1982 6.3 342.6 836.6 59.0 0.2 20.7 2.3 1147.3 4011.0 167.3
MC-1 07/07/1982 9.2 269.1 950.2 70.6 0.2 30.3 1.8 1395.8 3477.9 134.5
MC-1 09/07/1982 8.9 289.7 910.6 66.2 0.3 25.7 1.8 1357.6 23132.9 124.2
MC-1 22/07/1982am1 8.2 255.0 986.1 69.7 0.2 36.6 1.9 1504.6 1636.2 136.0
MC-1 22/07/1982pm2 7.3 255.0 833.0 62.9 0.4 35.7 1.7 1292.1 1734.0 119.0
MC-1 22/07/1982web1 8.0 240.7 945.5 68.8 0.2 37.8 1.9 1444.1 4707.6 128.9
MC-1 22/07/1982web2 7.7 282.9 923.6 68.2 0.3 38.3 1.8 1406.3 3941.8 124.8
MC-1 17/08/1982 1000 9.7 298.6 904.7 72.4 0.5 32.1 1.7 1464.0 2756.1 115.2
MC-1 10/09/1982 0900 8.0 303.3 713.1 60.7 1.1 109.8 1.1 1114.7 9575.9 172.1
MC-1 12/09/1982 0400 12.3 271.9 1174.7 85.6 0.3 50.3 1.9 1787.2 6014.1 184.6
MC-1 13/09/1982 1300 12.7 240.7 1160.4 90.3 0.5 78.2 1.9 1882.4 3380.6 128.9
MC-1 14/09/1982 1030 12.9 157.8 1218.2 97.8 0.6 67.4 2.4 1790.4 900.0 129.2
MC-1 14/09/1982 1100 12.6 155.4 1211.7 105.4 0.4 57.4 2.6 1831.4 914.5 129.5
MC-1 14/09/1982 1200 13.1 148.1 1238.8 98.7 0.4 50.3 2.5 1862.9 961.1 139.7
MC-1 14/09/1982 1100 11.1 169.0 1041.2 95.0 0.4 50.2 2.4 1634.8 1654.3 109.6
MC-1 14/09/1982 1130 12.6 153.0 1131.0 96.4 0.4 49.1 2.5 1770.7 1000.0 120.5
88
MC-1 25/09/1982 10.7 305.3 990.3 76.9 0.5 29.5 1.8 1579.6 2112.1 122.8
MC-1 27/09/1982 10.1 307.3 988.9 77.6 0.7 30.2 1.6 1585.6 1609.7 114.4
MC-1 01/10/1982 11.0 306.0 1030.7 81.0 0.8 30.3 1.9 1627.9 3016.8 114.5
MC-1 09/10/1982 11.6 193.9 1116.7 87.6 0.9 33.1 2.1 1724.2 1396.9 116.1
MC-1 18/10/1982 1200 10.6 316.6 1047.2 87.7 0.6 30.9 1.7 1680.3 2207.3 105.5
MC-1 23/10/1982 1200 10.5 303.3 1032.8 80.3 0.7 32.8 1.7 1631.1 2772.0 98.4
MC-1 24/10/1982 1200 10.7 316.6 1071.5 81.2 0.8 30.0 1.6 1647.8 4320.4 105.5
MC-1 25/10/1982 1200 11.1 323.1 1066.4 81.6 0.8 29.9 1.7 1648.0 4360.6 105.0
MC-1 28/10/1982 2400 6.3 283.0 615.8 49.1 0.7 27.5 1.5 907.1 1351.7 141.5
MC-1 29/10/1982 0800 9.5 303.3 926.2 75.4 0.8 38.5 1.6 1409.8 3274.6 131.1
MC-1 29/10/1982 2400 11.7 323.2 1163.6 92.1 1.2 66.3 1.9 1785.8 1384.0 153.5
MC-1 30/10/1982 0800 11.7 247.9 1119.8 86.3 3.9 63.3 1.7 1726.7 1161.9 145.3
MC-1 30/10/1982 2400 12.5 276.0 1187.8 88.7 16.7 53.5 2.2 1848.6 2320.3 158.9
MC-1 31/10/1982 0830 12.9 276.0 1237.9 105.4 19.2 54.4 2.3 1898.7 3598.9 142.2
MC-1 07/11/1982 1200 10.4 296.6 980.3 79.9 1.0 33.8 1.6 1598.1 1921.1 123.6
MC-1 09/11/1982 1200 9.9 282.9 973.6 79.1 1.0 30.8 1.5 1556.1 2698.2 108.2
MC-1 11/11/1982 0715 10.5 303.3 991.8 82.0 1.0 30.3 1.6 1631.1 2447.3 114.8
MC-1 11/11/1982 0945 10.9 316.6 990.3 81.2 1.1 30.0 1.6 1647.8 2714.8 105.5
MC-1 11/11/1982 0945 10.0 296.5 972.0 79.1 1.0 29.7 1.6 1598.0 2398.8 107.1
MC-1 15/11/1982 1200 7.2 196.2 668.7 54.4 1.5 32.1 1.2 1078.8 1876.6 76.7
MC-1 20/11/1982 1100 10.8 296.5 1046.1 82.4 1.0 30.5 1.6 1631.0 2370.0 107.1
MC-1 23/11/1982 1100 10.5 296.5 1046.1 82.4 1.1 29.7 1.6 1622.7 2334.8 107.1
MC-1 23/11/1982 1400 9.0 226.1 817.4 65.2 0.8 23.5 1.3 1295.7 7455.9 84.2
MC-1 28/11/1982am 10.9 303.3 1049.2 76.2 1.1 29.5 1.6 1631.1 2147.1 114.8
MC-1 01/12/1982pm 10.8 316.6 1039.0 75.5 1.1 30.1 1.6 1615.4 2318.9 105.5
MC-1 06/12/1982 1400 11.1 303.3 1040.9 76.2 1.1 29.9 1.6 1631.1 2635.0 114.8
MC-1 09/12/1982 1400 11.3 310.0 1027.7 75.0 1.1 29.8 1.6 1631.3 2092.0 114.2
MC-1 12/12/1982 1000 10.9 310.0 1027.7 75.9 1.1 29.4 1.6 1696.6 2201.3 114.2
MC-1 15/12/1982 0900 11.3 310.0 1035.9 75.0 1.1 29.0 1.6 1623.2 1793.4 114.2
89
MC-1 19/12/1982 0900 11.1 303.3 1049.2 76.2 1.1 29.5 1.6 1631.1 2089.8 114.8
MC-1 23/12/1982 0900 11.4 316.6 1063.4 89.3 1.3 29.2 1.7 1623.5 2502.0 105.5
MC-1 26/12/1982 1200 11.0 303.3 1057.4 90.2 1.2 30.3 1.7 1631.1 2383.3 106.6
MC-1 29/12/1982 1200 11.1 303.3 1057.4 92.6 1.1 37.7 1.7 1647.5 2362.2 114.8
MC-1 02/01/1983 1600 11.1 310.0 1052.4 89.7 1.1 30.2 1.7 1615.3 1674.2 114.2
MC-1 05/01/1983 1300 11.4 309.9 1035.9 91.4 1.1 29.4 1.6 1615.0 2920.6 106.0
MC-1 09/01/1983 0900 11.1 303.3 1040.9 96.7 1.1 29.5 1.6 1614.7 2854.6 98.4
MC-1 13/01/1983 1500 11.4 316.6 1039.0 90.9 1.1 29.2 1.6 1615.3 3002.6 97.4
MC-1 16/01/1983 1500 11.3 309.9 1044.0 96.3 1.1 29.4 1.6 1623.1 2927.2 97.9
MC-1 20/01/1983 1300 11.4 296.5 1054.4 98.9 1.1 31.3 1.6 1614.5 2345.3 98.9
MC-1 30/01/1983 0900 12.4 289.8 1142.5 103.5 1.0 37.3 1.7 1738.6 1943.8 107.6
MC-1 02/02/1983 1200 12.3 316.8 1234.5 95.0 0.6 47.1 2.0 1851.8 282.7 105.6
MC-1 06/02/1983 1730 11.3 289.8 1126.0 87.8 0.3 43.1 1.8 1597.9 1351.0 115.9
MC-1 09/02/1983 1500 10.5 296.5 971.9 79.9 3.1 45.3 1.6 1540.2 18855.3 98.8
MC-1 13/02/1983 2030 12.3 316.6 1152.8 89.3 0.2 36.5 1.9 1802.3 1272.8 113.7
MC-1 19/02/1983 1200 11.5 303.3 1082.0 86.9 0.9 32.0 1.8 1713.1 1896.3 123.0
MC-1 24/02/1983 0900 11.5 310.0 1084.9 87.3 1.1 31.0 1.8 1712.9 1649.8 114.2
MC-1 27/02/1983 0900 11.4 310.0 1052.2 88.9 1.1 31.0 1.7 1696.6 1651.8 130.5
MC-1 02/03/1983 1330 11.7 310.0 1060.4 95.4 1.2 31.8 2.3 1680.3 1555.8 106.0
MC-1 06/03/1983 0900 11.7 303.3 1090.1 95.1 1.2 32.0 2.2 1672.1 1967.8 106.6
MC-1 09/03/1983 0900 11.5 303.3 1082.0 93.4 1.2 32.0 2.2 1664.0 1565.4 106.6
MC-1 13/03/1983 0900 11.3 310.0 1076.7 88.9 1.1 32.6 2.3 1680.3 1653.4 106.0
MC-1 16/03/1983 0900 11.1 310.0 1068.6 90.5 1.2 31.0 2.2 1672.2 1619.5 106.0
MC-1 20/03/1983 0900 11.8 310.0 1044.1 89.7 1.2 31.8 2.2 1664.0 1597.7 106.0
MC-1 23/03/1983 0900 11.3 310.0 1052.2 93.0 1.2 31.8 2.2 1664.0 1613.7 106.0
MC-1 27/03/1983 0900 12.0 303.3 1073.8 92.6 1.2 32.8 2.2 1664.0 1550.8 106.6
MC-1 30/03/1983 12.2 310.0 1052.3 89.7 1.1 31.5 1.6 1680.4 1523.9 114.2
MC-1 03/04/1983 12.9 329.7 1141.9 96.5 0.4 33.7 1.8 1793.3 1690.3 112.6
MC-1 06/04/1983 12.1 329.7 1061.4 88.5 0.3 31.2 1.8 1712.8 2080.0 104.5
90
MC-1 10/04/1983 11.8 262.1 1116.0 93.0 1.2 31.8 1.7 1741.6 1597.3 118.4
MC-1 14/04/1983 11.5 303.3 1073.8 98.4 1.2 29.7 1.6 1663.9 1942.7 114.8
MC-1 18/04/1983 10.6 310.0 1044.1 89.7 1.3 29.5 1.6 1664.0 2025.2 114.2
MC-1 21/04/1983 11.4 310.0 1109.3 97.9 1.3 30.9 1.6 1647.7 2038.1 114.2
MC-1 24/04/1983 11.4 316.6 1022.8 89.3 1.3 29.2 1.5 1631.6 2053.1 113.7
MC-1 27/04/1983 11.4 316.6 1063.4 89.3 1.3 29.6 1.5 1639.8 2009.2 113.7
MC-1 01/05/1983 11.4 310.0 1044.1 89.7 1.3 29.5 1.6 1639.5 1998.6 114.2
MC-1 04/05/1983 12.2 310.0 1035.9 89.7 1.3 27.9 1.6 1639.5 1849.1 106.0
MC-1 08/05/1983 12.4 289.8 1068.0 91.1 1.3 29.8 1.6 1655.8 1806.9 115.9
MC-1 12/05/1983 0930 11.5 303.3 1049.2 82.0 1.2 28.7 1.8 1639.4 1945.7 114.8
MC-1 05/06/1983 0900 11.4 310.0 1101.1 89.7 1.2 27.7 1.8 1631.3 2341.0 106.0
MC-1 09/06/1983 0900 11.5 303.3 1024.6 82.0 1.2 27.9 1.8 1639.4 1988.4 98.4
MC-1 12/06/1983 0900 11.5 303.3 1016.4 82.0 1.2 27.9 1.8 1639.4 1864.2 123.0
MC-1 16/06/1983 11.5 303.3 1016.4 82.0 1.2 27.9 1.8 1647.5 2367.3 123.0
MC-1 19/06/1983 11.5 296.6 1021.4 82.4 1.2 28.0 1.8 1655.7 1929.7 123.6
MC-1 22/06/1983 11.3 323.2 1026.0 88.9 1.4 26.7 1.7 1623.9 2111.3 121.2
MC-1 26/06/1983 11.6 289.8 1051.4 91.1 1.3 27.3 1.7 1664.0 2141.4 132.5
MC-1 29/06/1983 11.6 289.8 1051.4 91.1 1.3 27.3 1.7 1655.8 1758.0 124.2
MC-1 03/07/1983 11.7 282.9 1048.5 91.5 1.3 26.6 1.7 1656.0 1704.6 124.8
MC-1 04/09/1983 12.9 240.7 1169.0 94.6 0.6 45.6 2.1 1830.9 2884.8 128.9
MC-1 11/09/1983 12.5 282.9 1140.0 91.5 0.8 40.8 2.1 1755.8 2808.7 99.9
MC-1 18/09/1983 12.4 296.5 1128.5 98.9 0.8 41.2 2.1 1754.5 2860.6 107.1
MC-1 09/10/1983 11.7 282.9 1098.5 99.9 1.2 30.0 2.1 1697.6 1623.9 108.2
MC-1 16/10/1983 11.7 276.0 1087.4 100.4 1.3 30.1 2.0 1698.1 1534.8 108.7
MC-1 23/10/1983 11.6 282.9 1048.5 91.5 1.2 29.1 2.1 1689.2 1895.6 116.5
MC-1 05/12/1983 0900 12.5 196.2 1185.9 107.0 1.2 30.3 1.8 1275.1 610.9 78.5
MC-1 05/12/1983 9.5 233.4 899.2 77.8 1.0 22.5 1.4 1755.1 1449.5 121.0
MC-1 11/12/1983 0900 10.3 240.7 943.9 79.1 0.9 23.2 1.5 1143.3 842.1 71.4
MC-1 11/12/1983 10.1 269.1 992.2 84.1 1.1 24.4 1.5 1698.6 1742.8 126.1
91
MC-1 18/12/1983 0900 10.3 240.7 902.6 76.5 0.9 23.2 1.5 1727.8 1471.1 111.8
MC-1 18/12/1983 8.7 226.1 852.3 74.8 1.0 21.7 1.3 1348.0 1176.3 104.4
MC-1 25/12/1983 0900 12.5 282.9 1081.8 91.5 1.2 25.8 1.7 1681.0 1719.3 108.2
MC-1 25/12/1983 10.7 296.5 1062.6 90.6 1.2 27.2 1.6 1672.2 2048.2 115.3
MC-1 01/01/1984 0900 11.7 282.9 1073.5 91.5 1.1 26.6 1.7 1672.6 1742.7 108.2
MC-1 01/01/1984 10.8 289.8 1068.0 91.1 1.2 26.5 1.7 1680.6 1545.8 115.9
MC-1 12/01/1984 0900 11.6 289.8 1076.3 91.1 1.2 26.5 1.7 1664.1 1798.8 107.6
MC-1 15/01/1984 11.6 289.8 1084.5 91.1 1.2 27.3 1.7 1680.6 1868.6 115.9
MC-1 22/01/1984 0900 11.6 289.8 1084.6 91.1 1.1 25.7 1.7 1672.4 1761.1 107.6
MC-1 22/01/1984 11.6 289.8 1084.6 91.1 1.1 27.3 1.7 1672.4 1562.0 115.9
MC-1 29/01/1984 0900 12.4 296.6 1062.6 90.6 1.1 25.5 1.7 1655.7 1830.0 107.1
MC-1 29/01/1984 11.0 262.1 1039.8 76.9 0.8 38.9 1.7 1699.2 1933.5 118.4
MC-1 15/07/1984 12.4 296.6 1128.8 98.9 0.7 30.5 1.6 1763.2 639.5 107.1
MC-1 25/07/1984 12.4 296.6 1128.8 98.9 0.7 28.8 1.8 1779.7 551.5 107.1
MC-1 31/07/1984 12.4 296.6 1120.3 98.9 0.7 31.3 1.7 1771.1 1291.9 107.1
MC-1 09/08/1984 12.4 296.6 1136.8 98.9 0.7 31.3 1.8 1771.1 1250.4 107.1
MC-1 15/08/1984 12.3 303.3 1123.0 98.4 0.7 31.2 1.9 1754.2 1201.2 98.4
MC-1 23/08/1984 12.3 303.3 1123.0 98.4 0.7 31.2 1.9 1762.3 1625.0 98.4
MC-1 31/08/1984 13.2 296.6 1128.6 107.1 0.7 30.5 1.9 1771.1 1557.6 98.9
MC-1 06/09/1984 12.3 303.3 1114.8 98.4 0.7 31.2 1.9 1754.1 1625.2 98.4
MC-1 13/09/1984 12.3 303.3 1106.7 98.4 0.7 30.3 1.9 1754.4 808.4 98.4
MC-1 20/09/1984 12.3 303.3 1114.8 98.4 0.7 31.2 1.9 1754.1 1541.9 98.4
MC-1 28/09/1984 12.3 303.3 1131.2 106.6 0.7 30.3 1.9 1754.1 1584.7 98.4
MC-1 04/10/1984 11.5 296.6 1112.1 107.1 0.7 30.5 1.9 1762.8 1561.2 98.9
MC-2 03/06/1982 4.9 211.3 651.5 63.4 3.8 29.1 0.7 871.5 2478.6 176.1
MC-2 22/10/1982 0800 2.7 226.1 347.9 24.4 1.3 43.5 0.7 504.5 586.8 156.6
MC-2 23/10/1982 1000 5.4 342.6 557.7 46.2 1.4 46.2 1.2 852.5 1715.4 127.5
MC-2 24/10/1982 1400 7.5 348.9 650.3 61.1 1.4 43.6 1.2 1062.7 11277.4 126.9
MC-2 25/10/1982 0600 8.2 367.9 743.7 72.8 0.5 38.4 1.3 1166.4 1095.4 117.4
92
MC-2 13/11/1982 1000 11.0 233.4 1002.9 79.5 5.7 112.4 1.3 1573.5 1490.0 155.6
MC-2 13/11/1982 1400 16.8 269.7 1693.9 151.7 5.3 118.0 2.2 2536.6 243.2 353.9
MC-2 13/11/1982 1600 10.3 329.7 892.6 74.0 7.3 80.4 1.4 1415.3 1702.2 128.7
MC-2 13/11/1982 1800 10.3 342.6 948.1 82.9 13.5 143.4 1.8 1513.8 1024.4 151.4
MC-2 13/11/1982 1900 49.6 124.1 5010.4 429.5 2.1 725.3 6.9 7921.2 2420.0 1336.1
MC-3 16/10/1982 1900 5.0 283.0 641.0 43.3 0.7 26.6 1.4 707.6 1152.8 349.6
MC-3 20/10/1982 1600 8.4 361.4 947.7 62.6 2.2 85.1 2.1 1092.3 170.8 473.8
MC-3 21/10/1982 1000 8.3 226.1 982.8 68.7 2.5 22.6 1.0 408.8 2772.5 347.9
MC-3 25/10/1982 2000 1.4 211.3 255.3 23.8 1.7 44.0 0.6 220.1 2461.8 325.7
MC-3 26/10/1982 0400 2.8 247.9 384.6 31.6 1.5 22.2 0.9 384.6 3240.7 333.4
MC-3 26/10/1982 2000 5.0 310.3 661.4 49.8 1.9 96.4 1.5 734.8 693.3 449.1
MC-3 27/10/1982 0900 4.3 269.1 529.8 42.9 2.0 23.6 1.0 630.7 2635.4 328.0
MC-3 28/10/1982 1000 6.1 248.0 684.1 50.5 0.8 10.3 1.0 820.9 626.4 333.5
MC-3 02/11/1982 1400 5.6 269.1 647.6 47.9 1.3 16.8 1.1 798.9 1962.5 302.8
MC-3 02/11/1982 2200 6.1 276.0 669.2 48.5 1.8 20.9 1.2 803.0 3130.2 326.2
MC-3 09/11/1982 1200 7.4 283.0 799.0 58.3 1.2 15.8 1.1 1106.9 2088.8 283.0
MC-3 09/11/1982 2000 8.0 240.8 834.1 56.8 1.6 24.9 1.5 1092.0 968.6 335.4
MC-3 11/11/1982 1436 8.4 255.1 824.7 60.4 0.7 11.1 1.2 1088.3 1639.3 297.6
MC-3 11/11/1982 1834 8.5 211.4 889.4 62.5 1.1 30.8 1.7 1206.4 647.1 361.1
MC-6 2230 3.6 149.7 724.4 40.9 3.8 62.6 302.2 8227.2 421.3
MC-6 40 4.4 192.3 776.5 52.6 5.7 61.5 400.8 10539.1 356.0
MC-6 515 7.4 111.9 1183.7 86.1 1.3 50.9 778.1 6332.8 405.6
MC-6 745 8.1 120.9 1201.6 91.4 0.2 51.8 771.7 23789.7 383.6
MC-6 6.1 97.9 878.9 69.6 0.2 48.8 686.9 5110.0
MC-8 (Thermochem Air Lift
Analysis, 2008) 13851-2 14.7 462.1 1291.1 200.3 0.0 33.8 1.7 2164.0 6279.0 67.2
MC-8 (Thermochem Air Lift
Analysis, 2008) 13851-3 14.8 456.0 1267.0 205.5 0.0 34.9 1.7 2180.4 6005.1 65.9
MC-8 (Thermochem Air Lift
Analysis, 2008) 13851-4 15.8 408.0 1316.8 212.4 0.2 47.7 1.7 2306.2 3582.4 71.0