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This version was published on November 1, 2009
GSA Bulletin; November 2009; v. 121; no. 11-12; p. 1570-1583; DOI: 10.1130/B26305.1
© 2009 Geological Society of America
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High-resolution seismic and resistivity profiling of a buried Quaternary subglacial valley: Northern Alberta, Canada

Jawwad Ahmad1, Douglas R. Schmitt1,{dagger}, C. Dean Rokosh1,2 and John G. Pawlowicz2

1 Institute for Geophysical Research, Department of Physics, Mailstop #615, University of Alberta, Edmonton, Alberta T6G 2G7, Canada
2 Alberta Geological Survey, 4th Floor, Twin Atria Building, 4999-98 Ave. NW, Edmonton, Alberta T6B 2X3, Canada

Correspondence: {dagger}E-mail: doug{at}phys.ualberta.ca or doug.schmitt{at}gmail.com


    ABSTRACT
 TOP
 ABSTRACT
 INTRODUCTION
 BACKGROUND
 GEOLOGICAL BACKGROUND
 METHODS AND FIELD PROGRAM
 RESULTS
 DISCUSSION
 CONCLUSIONS
 REFERENCES CITED
 
High-resolution seismic and resistivity profiles were acquired to assist in the delineation of a buried Quaternary subglacial valley, the existence of which was first discovered by drilling. One aspect of this valley is the glacial sediments that host substantial methane at shallow depths (~50 m or less). Geophysical well logs indicate that the glacial sediments in this area generally have lower compressional wave speeds VP <1800 m/s and greater electrical resistivity r >10 {Omega}·m than adjacent undisturbed Cretaceous-age rocks, which have VP >2200 m/s and r <10 {Omega}·m, respectively. Seismic-refraction velocities, seismic-reflection architecture, and electrical resistivity tomography images all indicate a deep (>300 m) valley. The reflection profile reveals a complex series of events consistent with heterogeneous deposition. One major reflection dips eastward across the valley. The reflection character changes abruptly on either side of this event, with dipping clinoform reflections beneath and nearly horizontal reflections above. These may be related to changes in deposition processes beneath a retreating ice sheet, as has been suggested by earlier workers. The buried valley's basal reflections are complex and possibly reflect glaciotectonic deformation or block plucking. The near-surface methane gas is within, but at the edge of, the valley. The methane gas–saturated zone displays anomalously high resistivities both in the well logs and in resistivity tomography.


    INTRODUCTION
 TOP
 ABSTRACT
 INTRODUCTION
 BACKGROUND
 GEOLOGICAL BACKGROUND
 METHODS AND FIELD PROGRAM
 RESULTS
 DISCUSSION
 CONCLUSIONS
 REFERENCES CITED
 
Buried, subglacial tunnel valleys are important because they contain aggregates for construction, host substantial groundwater reserves for human or industrial uses, direct the movement of contaminants in groundwater, hold clues to Earth's Quaternary climate, and even store economic reserves of methane. Such features exist in many of the recently glaciated, lowland regions of the world. The study of such valleys has advanced a great deal in recent years, particularly in northern Europe, where the demands of a dense population stress both the supply and the quality of groundwaters. Geophysical investigations of such buried structures in North America as are not as extensive, despite similar pressures.

Such valleys lie near the surface, but they often have no obvious geomorphologic surface expression, and they are difficult to both find and delineate. Indeed, many such features are only found by serendipitous water-well drilling. However, it is expensive to delineate buried valleys on the basis of drilling alone; geophysical investigations are of great utility in further outlining such structures.

This contribution provides the results from an integrated geological and geophysical profiling of one such buried valley in northern Alberta, Canada, from the initial discovery of the valley from geophysical well logs via the contrasts in physical properties, through refinement of the location of the valley with seismic-refraction profiling, and finally to delineation of the architecture of the buried valley with both seismic-reflection and electrical resistivity tomography (ERT) profiles (Ahmad, 2006). The structure of the valley, particularly as revealed in the seismic-reflection profile, may hold clues to the subglacial processes active beneath retreating ice sheets. Similar features are seen in studies of buried valleys in the North Sea and indicate that the same subglacial processes acted in both locales.


    BACKGROUND
 TOP
 ABSTRACT
 INTRODUCTION
 BACKGROUND
 GEOLOGICAL BACKGROUND
 METHODS AND FIELD PROGRAM
 RESULTS
 DISCUSSION
 CONCLUSIONS
 REFERENCES CITED
 
This section provides an overview of the literature as it pertains to glacially related buried valleys, with some focus on geophysical investigations of such features. A short review of known occurrences of methane gas within buried valleys is also provided

Tunnel Channels and Valleys
Advances and retreats of continental ice sheets dramatically alter Earth's surface. River valleys that predate glaciation and tunnel valleys contemporaneous with glaciation (O'Cofaigh, 1996; Shaw, 2002) are often filled by tills and glacial lake sediments (e.g., Ehlers and Linke, 1989; Huuse and Lykke-Andersen, 2000; Praeg, 2003; Jorgensen and Sandersen, 2006). Pleistocene buried valleys abound in the glaciated mid latitudes of North America and Europe, and much older fossil valleys have even been located at various locales such as Jordan, Australia, and Niger (e.g., Eyles and de Broekert, 2001; Denis et al., 2007). Hooke and Jennings (2006) summarized a number of characteristics that distinguish tunnel valleys, among which are their dimensions, which are typically from 5 to 20 km long, 150 to 500 m wide, and ~5 to 30 m deep (although, usually, the depth of the valley fill is unknown). However, larger dimensions up to many tens of kilometers, kilometer-scale widths, and hundreds of meters of depth are at least as common in the literature (e.g., Piotrowski, 1994; Huuse and Lykke-Andersen, 2000). For example, Kristensen et al. (2007) recently carried out, using three-dimensional (3-D) seismic volumes, a detailed analysis of the basal geometry of a series of buried channels in the North Sea off of Denmark. The valleys were typically 3–4 km wide, up to 350 m deep, and as long as 39 km. Their bottom topography undulates, creating subbasins and thresholds, and an adverse end slope is seen at their termination. This complex morphology suggests that the buried valleys were created by subglacial flow linked to the still poorly understood hydrological processes both beneath and outboard of continental glaciers (Brennand and Shaw, 1994; Huuse and Lykke-Andersen, 2000; Beaney, 2002), but likely including a combination of erosion by uniform flow, catastrophic discharge, and glacial ice abrasion and plucking (e.g., Praeg, 2003; Jorgensen and Sandersen, 2006; Lonergan et al., 2006).

Further, areal geophysical seismic and electromagnetic (EM) surveys reveal that tunnel valleys appear in three dimensions together in complex anastamosing and crosscutting patterns (Huuse and Lykke-Andersen, 2000; Kluiving et al., 2003; Praeg, 2003; Lonergan et al., 2006; Kristensen et al., 2007). Upon even closer examination, a given valley appears to be constructed of numerous generations of cut-and-fill structures (Jorgensen and Sandersen, 2006; Jørgensen and Sandersen, 2008), suggesting that the valleys had been eroded and filled many times.

A clear definition of the differences between channels and valleys is required, and here we use the terminology as reviewed recently by Fisher et al. (2005, p. 2377) (see also Clayton et al., 1999; Jorgensen and Sandersen, 2006). A tunnel channel is a depression formed by a "subglacial bankfull discharge, where the size of the channel matches the size of the valley." In contrast, a tunnel valley is excavated by horizontal and vertical migration of a tunnel channel scouring out the final valley.

The valley fill consists of complex packages of weakly consolidated glaciofluvial and glaciolacustrine sands, gravels, boulders, and clays as observed from well logs (e.g., Kluiving et al., 2003), cores (e.g., Russell et al., 2003), or directly in exposures (e.g., Ehlers, 2005; Fisher et al., 2005). Munro-Stasiuk (2003), for example, classified six different facies that depend to a large degree on whether sedimentation occurred during advance of, during (and hence beneath), or upon retreat of glaciation.

Glacially filled incised valleys are common both onshore and offshore in northern Europe. There are numerous studies published in the open literature, primarily because of the need for groundwater resources in those densely populated regions (e.g., Huuse et al., 2003). Buried valleys are also common in North America, which is represented by a large body of geomorphological and geological literature (e.g., Boyd et al., 1988; Sharpe et al., 1992; Brennand and Shaw, 1994; Clayton et al., 1999; Cutler et al., 2002; Russell et al., 2003; Hooke and Jennings, 2006; Ross et al., 2006), a complete review of which is beyond the scope of this contribution. In contrast to the European situation, however, in North American public domain geophysical surveys over such features are rare.

In Alberta and Saskatchewan, the existence of such buried valleys was known almost from the first geological explorations along the river valleys where exposures may be seen, and location of groundwater resources within them has been particularly important in the arid southern portions of these provinces. Stalker (1960) provided details of the location and character of the numerous buried valleys of central and southern Alberta and correlated the current and preglacial drainage patterns; this early work was followed by numerous later studies (Rains et al., 2002; Sjogren et al., 2002; Munro-Stasiuk, 2003). In northeastern Alberta, Andriashek and Atkinson (2007) used data from more than 30,000 wells to map buried valleys and glacial-drift aquifers in the extensive oil sands region.

Geophysical Investigations of Buried Channels and Valleys
While not focusing on buried valleys directly, there are also numerous geophysical studies of glacially derived sediments that are worth mentioning because they demonstrate that glacial deposits are not easily characterized (e.g., Roberts et al., 1992; Keiswetter et al., 1994; Buker et al., 2000; Nitsche et al., 2002; Eyles et al., 2003; Kilner et al., 2005; Ross et al., 2006; Smith and Sjogren, 2006). Their architecture can be highly heterogeneous and include a wide variety of sediment types from gravels to clays with different geophysical properties.

The overwhelming majority of geophysical studies of buried valleys come from northern Europe. A recent special issue of the Journal of Applied Geophysics provides an extensive overview of a number of geophysical investigations of buried valleys (Huuse et al., 2003), and the northern European BurVal Working Group recently released an extensive report (Kirsch et al., 2006) on locating groundwater resources in buried glacial valleys.

A wide variety of geophysical techniques have been employed, ranging from gravity (Gabriel et al., 2003; Gabriel, 2006; Møller et al., 2007), which searches for density contrasts, to ground-penetrating radar (Fisher et al., 2005), which images the detailed structure of the near-surface fill material. However, seismic, DC electrical, and electromagnetic (EM) methods are the most popular. High-resolution seismic images have been used for groundwater exploration (Buker et al., 1998; Wiederhold et al., 1998; Holzschuh, 2002; Jorgensen et al., 2003; Bergman et al., 2004) or to image glacial deposits and glacial basins (Pugin and Rossetti, 1992; Bradford et al., 1998; Musil et al., 2002). Both ground-based (Baines et al., 2002; Jorgensen et al., 2003; Thomsen et al., 2004; Kilner et al., 2005; Jorgensen and Sandersen, 2006; Bersezio et al., 2007) and airborne electromagnetic (Sørensen and Auken, 2004; Eberle and Siemon, 2006) techniques have also been extensively employed.

Arguably, however, marine seismic-reflection surveys provide some of the best information regarding both the regional configurations of buried valleys and their internal structure. Near Sable Island off the east coast of Nova Scotia, Boyd et al. (1988), some of the first workers to exploit commercial seismic data acquired for petroleum exploration, regionally mapped the pattern of tunnel valleys and showed the details of their interior structure. Huuse et al. (2001) interpreted over 6400 km of specially acquired high-resolution marine two-dimensional (2-D) profiles supplemented with over 18,000 km of conventional 2-D profiles to map Quaternary valleys offshore west of Jutland. Kluiving et al. (2003) interpreted a series of 2-D profiles in the North Sea off of the Netherlands. Eiriksson et al. (2006) also acquired 2-D profiles in the constricted southern Lillebælt marine area in eastern Denmark, and they were able to image and map buried valleys. Most recently, Halliday et al. (2008) interpreted marine seismic and multibeam sonar data to highlight the effects of methane within glacial sediments off the coast of British Columbia. Data from large 3-D marine surveys covering areas in excess of 1000 km2 and originally acquired for petroleum exploration in deeper prospective formations in the North Sea have also been profitably reprocessed and interpreted to highlight the overlapping geometry of successive episodes of tunnel valley formation during the Pleistocene (Praeg, 2003; Lonergan et al., 2006; Kristensen et al., 2007, 2008; Kuhlmann and Wong, 2008). Praeg (2003) also provided a comprehensive review of earlier literature. The topography of a series of valleys extracted from 3-D data by Kristensen et al. (2007) shows undulating bottoms and adverse end slopes that are generally characteristic of subglacial valleys.

In western Canada, geophysical investigations of buried valleys began early with gravity (Hall and Hajnal, 1962), electrical resistivity (Lennox and Carlson, 1967), and seismic methods (Hobson et al., 1970) all being employed. More recently, seismic methods have been used to characterize Quaternary sediments (Francese et al., 2002). Langenberg et al. (2002), as part of a study of the detailed structure of oil sands, provided a seismic profile that also coincidentally includes a buried Quaternary valley.

Shallow Gas
One additional factor that makes buried valleys interesting is that the complex geological structure may both contain and trap hydrocarbon gas, in some cases, in economic concentrations. Such "Quaternary" gas has been produced from different parts of China for many centuries (Kuhn, 2004). Indeed, wellbore drilling was developed there to exploit near-surface gas and associated brines that together were used in the manufacture of salt on a large scale. Major Quaternary biogenic gas fields are found in Qaidam Basin and the Yangtze River delta near Shanghai (Jianyi et al., 1999). Recently, several Quaternary shallow (30–55 m) gas pools have also been discovered and produced in China in the province of Zhejiang (Lin et al., 2004). These gas pools are generally located in deeply incised valleys filled with highly porous fluvial sediments.

Methane has been detected in the marine seismic surveys in northern Europe. Such gas can be problematic for seismic imaging, first because of its low velocity and associated distorting "pull-down" effects on deeper reflections, and second due to the loss of signal beneath such gas-filled zones, referred to as "acoustic turbidity" or "blanking" (Eiriksson et al., 2006; Halliday et al., 2008). The gas-saturated zones will also produce strong "bright spot" reflections (Kuhlmann and Wong, 2008).

Glacial deposits are also known to host modest economic gas reserves in North America, such as in Pointe-du-Lac, Québec, and Bouttineau County, North Dakota (Anderson et al., 2006). Commercial amounts of gas have been produced from glacial deposits of the Rainbow and the Sousa fields in northern Alberta (Pawlowicz et al., 2004), and local "permanent" burning gas seeps occur near the current study area (Letourneau et al., 2000). These fields lie to the west between High Level and Rainbow Lake, Alberta (Fig. 1). In these fields, the gas lies at depths of <100 m; this creates a substantial hazard during drilling of water or deeper hydro carbon wells, and disastrous blowouts have occurred as recently as 2005.


Figure 01
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Figure 1. (A) The general study area in northwest Alberta is marked by the large star in the top panel (~58°35'N, ~118°31'W). N.W.T.—Northwest Territory. (B) The detailed panel shows both the locations according to legal Section-Range-Township system of the Dominion Land Survey (DLS) (see McKercher and Wolfe, 1986); thick and thin gray lines delimit individual townships and sections, respectively. Thin black lines are the corresponding latitude and longitude. The black dashed line gives the location of the coincident 10-km-long seismic and the shallow electrical resistivity tomography (ERT) profile. The seismic reference field stations number 0–2400. The location numbers along this profile are referenced with respect to the common midpoint (CMP) number of the traces in the seismic profile. The locations of shallow methane gas production wells in the Rainbow field are marked by black dots. The arrows point to the locations of the in-channel (IC) and outside-channel (OC) wells from which the comparison geophysical logs of Figure 3 are taken. SC—Sousa Creek. (C) Contour map of the bedrock topography as derived from Pawlowicz et al. (2005a, 2005b) with the location of the seismic and shallow ERT profiles shown as a black line. Small circles are locations of boreholes that provided the data used to determine the elevation of the top of the bedrock. Contours are the elevation of the bedrock surface in meters from sea level. Scale is the same as in B.

 
While such shallow gas often results from biological activity, the chemical signature of the shallow gas in the present study area has a deeper thermogenic chemical signature (Letourneau et al., 2000). The carbon isotopic and heavy hydrocarbon ratios of the gas indicate that it is the same as that found in a Cretaceous-age formation (Letourneau et al., 2000), regionally referred to as the Bluesky, that is here cut by the valley. This suggests that gases migrated from these deeper bedrock formations to be trapped within the porous glaciofluvial sediments.


    GEOLOGICAL BACKGROUND
 TOP
 ABSTRACT
 INTRODUCTION
 BACKGROUND
 GEOLOGICAL BACKGROUND
 METHODS AND FIELD PROGRAM
 RESULTS
 DISCUSSION
 CONCLUSIONS
 REFERENCES CITED
 
Geological Framework
The study area containing the buried valley (Fig. 1) is located in the extreme northwest corner of Alberta, Canada. The area falls between the lowlands bounded to the north by the Cameron Hills, to the south by the Clear Hills, and to the east by Caribou Mountains. Aside from the filled valleys, the area is mostly blanketed at the surface by the glacial deposits likely left from the last retreat of the Wisconsin glaciation ~10,000 a ago (e.g., Shaw, 2002). Beneath this, the pre-Quaternary bedrock consists of Cretaceous (ca. 100 Ma) sandstone-shale sequences above Mississippian–Late Devonian (ca. 340 Ma) carbonates, which are underlain by a thick succession of Middle Devonian (ca. 380 Ma) shale. The unconformity between the Paleozoic carbonates and the Cretaceous siliciclastic rocks will hereafter be referred to as the sub-Cretaceous unconformity and denoted pK; this will also be applied to sections of the current profiles in the valley where the entire Cretaceous section has been eroded and Quaternary sediments contact the Paleozoic bedrock directly. The incised valley filled with Quaternary sediments cuts both the Cretaceous and the Paleozoic rock, making the contacts at the base of the Quaternary sediments unconformable. This unconformity has been interpreted from the existing geophysical well logs, and the bedrock topography is mapped on this basis (Fig. 1C) (Pawlowicz et al., 2005a, 2005b). The upper portions of the geology are shown in the generalized stratigraphic chart (Fig. 2). It must be noted that the well-log and drill-cutting information through the valley-fill materials is of insufficient lateral and vertical detail to allow for more than a broad characterization of the sediments, primarily because it normally is of no interest to petroleum drilling.


Figure 02
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Figure 2. Generalized stratigraphic column to the bottom of the Upper Devonian based on regional correlations and wells nearby to the survey site. Mississippian unconformity separates the Carboniferous Banff sequence from the Aptian Gething (GTH) to Lower Albian Bluesky (BLS) Formations. Formations overlying Lower Albian Spirit River include the Wilrich (WLR), Fahler, and Notikewin (NTK) Members. The Middle and Upper Albian Peace River Formation (PRV) is separated from the Upper Albian Shaftesbury (SFB) Formation by an Upper Albian unconformity. Outside of the valley, the glacial sediments lie unconformably above the Shaftesbury Formation, and at the deepest point within the valley, glacial sediments lie above the Devonian Wabamun Group.

 
The Quaternary valley-fill sediments mainly consist of a series of alternating layers of till and coarse-grained stratified sediments (Fenton et al., 1994). The retreat of the last ice sheet in northeast British Columbia and adjacent Alberta and the associated geomorphology of melt water valleys and ice-dammed lakes are described in Mathews (1980). In this region, two different types of valley systems are identified: (1) broad, shallow-walled valleys, which represent old Tertiary or Cretaceous river systems, and (2) steep-walled meltwater valleys, which formed during the Quaternary glaciations. These horizontally isolated, stacked meltwater valleys are separated by layers of till and are good traps because the fine-grained till and perhaps clay-rich lake sediment provide an excellent low-permeability seal. Both types of paleovalleys are deeply incised into the Cretaceous strata and, at the study location, even into the top of the Devonian Wabamun Formation. These valleys are filled with up to 300 m or more of drift, which consists of till, glaciolacustrine, and glaciofluvial sediments, and, for the older valleys, preglacial fluvial sediments (Pawlowicz et al., 2004).

Physical Properties from Geophysical Logs
Some of the properties of the glacial and sedi mentary lithologies both within and outside of the buried valley were obtained from geophysical logging. Details of each logging method are beyond the scope of this paper; for the physics of such logging tools, readers are referred to Hearst et al. (2000) or Ellis (1987), and to Darling (2005) for interpretation and geological applications of such logs. The geophysical logs shown (Fig. 3) were obtained from the publicly available petroleum well-log databases for western Canada. The data were obtained by various geophysical contractors at the time the wells were drilled.


Figure 03
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Figure 3. Composite natural gamma-ray (A), sonic compressional wave velocity (B), electrical resistivity in logarithmic scale (C), and density (D) logs indicated by the black line for the inside-channel (IC) borehole (well: 102/012011003W6 in Dominion Land Survey of Canada [DLS] system) and by gray fill for the outside-channel (OC) borehole (well: 100/010611103W6 in DLS system). Gray K represents the top of the Cretaceous section in the OC borehole, while gray and black D represents the depth of the sub-Cretaceous unconformity in the OC and the IC boreholes, respectively.

 
The typical log characters between one key valley-fill well (IC) and one contrasting nonvalley-fill well (OC) are compared in Figure 3; the drift thickness or the depth to the top of the bedrock is ~350 m to 360 m (to the top of the Paleozoic carbonate bedrock) and 130 m (to the top of the Cretaceous siliciclastic bedrock), respectively. Both of these wells show the difference in the physical properties of valley fill relative to the Cretaceous bedrock.

Both the Quaternary and pre-Quaternary sediments are also easily differentiated on the gamma-ray (GR) log (Fig. 3A). The gamma-ray value of the clay-rich siliciclastic Cretaceous bedrock outside the valley is high (>200 American Petroleum Institute units), and it is generally substantially lower (~50 API) in the valley-fill glacial sediments. In both wells, the GR data are unreliable in the Paleozoic carbonates below 355 m depth because these boreholes do not extend into this formation. The sonic log (Fig. 3B) also shows discernible differences between the three distinct units. The Paleozoic carbonates are clearly evident in the out-of-valley (OC) well by their high velocity (>4500 m/s). Unfortunately, there are no sonic log values above 230 m depth for the in-valley (IC) well. However, the velocities of the Quaternary sediments (~1500 m/s to 2000 m/s) can be easily distinguished from the Cretaceous bedrock (>2200 m/s). The Quaternary sediments are generally substantially more electrically resistive (>10 {Omega}·m) than the older Cretaceous bedrock (<10 {Omega}·m) (Fig. 3C). This difference is likely due to the higher conductivity of the clay-rich, predominantly marine Cretaceous rock. The Quaternary deposits, in contrast, contain greater proportions of clean sands and gravels that are filled with freshwater and maybe even insulating free gas. The lack of clays within the Paleozoic carbonates below ~355 m depth may be a reason for their high resistance (~50 {Omega}·m). Consequently, the Quaternary, the Cretaceous, and the Paleozoic units are all clearly distinguished on the basis of their resistivity for the OC well. The absence of the Cretaceous unit is evident by the high resistivity throughout the entire depth of the IC well. The bulk densities range between 2.0 g/cm3 and 2.5 g/cm3 (Fig. 3D). A discontinuous jump in the density is seen across the sub-Cretaceous unconformity on the OC log, but it is not clearly seen on the IC log. Differences are more subtle in this log. As expected, the densities of the upper Quaternary sections in both logs are similar. Beneath the pre-Quaternary discontinuity in the OC log, the density of the Cretaceous rocks generally exceeds that of the fill material in the valley. The differences, however, are small, and interpretation of the valley versus the nonvalley materials on the basis of the density log is difficult.

The geophysical logs of Figure 3 illustrate the physical property differences between the water-saturated valley fill and the older Cretaceous and Paleozoic bedrock. It is interesting, however, to also compare the rare log acquired through a shallow gas-saturated zone (Fig. 4), since the differences here will also show up as a geophysical anomaly in the surface surveys carried out in this study. The producing gas-saturated zone, highlighted by gray overlay from 64 m to 72 m depth (Pawlowicz et al., 2004), is clearly apparent only in the resistivity log, which shows a reading generally in excess of 30 {Omega}·m, with some values exceeding 100 {Omega}·m. Such high values are anomalous and indicate the presence of insulating pore fluids. A small highly resistive anomaly (100 {Omega}·m) at 100 m depth in the IC log may also be indicative of free gas. The resistive zone is not clearly visible in the other logs in Figure 4, although there appears to be a drop in the sonic velocity and a discontinuity in the natural gamma-ray logs below 63 m depth. The sonic velocity through the zone (~1600 m/s to 1700 m/s) of Figure 4 also appears lower than in the nearby IC log (~1800 m/s to 1900 m/s) in Figure 3. There is insufficient information to know to what degree gas may saturate the formation below the producing interval, but the resistivity remains high (>30 {Omega}·m) and the sonic velocity remains low below 72 m; this may be suggestive of additional partial-gas saturation in the fill material.


Figure 04
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Figure 4. Geophysical logs for a well intersecting a near-surface (~64 m to 74 m depth as indicated by gray fill) gas deposit (well: 100/011711003W6 in Dominion Land Survey of Canada system). (A) Natural gamma ray log. (B) Density (broken line) and sonic compressional wave velocity (continuous line). (C) Electrical resistivity, logarithmic scale.

 

    METHODS AND FIELD PROGRAM
 TOP
 ABSTRACT
 INTRODUCTION
 BACKGROUND
 GEOLOGICAL BACKGROUND
 METHODS AND FIELD PROGRAM
 RESULTS
 DISCUSSION
 CONCLUSIONS
 REFERENCES CITED
 
The deployment of the instruments and the raw and processed results are covered in this section. The methods employed include high-resolution seismic refraction and reflection (e.g., Brouwer and Helbig, 1998; Baker, 1999) and electrical resistivity tomography (ERT) (e.g., Baines et al., 2002; Daily et al., 2005; Bersezio et al., 2007).

Seismic Measurements
The field area was selected on the basis of analysis of existing well logs that suggested the existence of a deep valley. The availability of earlier ERT soundings and preexisting seismic clearings cut through the forest were also taken into consideration when designing the program. The goal of the survey was to image the structure above the sub-Cretaceous unconformity that lies at depths of ~350 m to 360 m, and as such, a nonstandard acquisition program employing both close spatial group spacing (4 m) and high frequencies was employed. High-frequency (40 Hz) geophones were selected to attenuate both ground roll and potential noise from the nearby highway. Based on our field experiences, the loss of the signal's frequency content below 40 Hz is more than compensated by the boost in the relative strength of the near-surface reflections, primarily because of the attenuation of the surface waves. These acquisition parameters are similar to some land-based studies (Wiederhold et al., 1998; Jorgensen et al., 2003) but generally are of smaller lateral spatial resolution than most marine 3-D studies, which are able to take advantage of existing commercial seismic data acquired in petroleum exploration.

The ground roll was further reduced by using an 8 s linear vibrator sweep beginning at 20 Hz through to 250 Hz produced with a high-frequency MinivibTM unit (Industrial Vehicles International of Tulsa, Oklahoma). A 240-channel semidistributed GeodeTM seismograph (Geometrics Ltd., San Jose, California) acquired the raw seismic traces. High spatial resolution was maintained by using geophone singles at 4 m station spacing. The vibration point spacing of 24 m (six stations) was a compromise between the maximum number of shots (up to 150) that could be carried out during the shorter daylight hours and the desire to maximize midpoint fold. An average fold of 40 was obtained for the survey. Upon completion of the survey, the data were archived in a SEGY format with geometry in UTM coordinates.

The raw seismic-reflection data were processed using the standard common midpoint (CMP) method (e.g., Yilmaz, 2001) with a commercial seismic data-processing package (Vista® by GEDCO, Calgary). The procedures for processing of near-surface seismic data differ in many respects from usually much deeper conventional petroleum exploration. For example, the final common midpoint trace spacing in this study was only 4 m, and only geophone singles were used in the acquisition (but with 4-m-long CMP bins averaging the response of two geophones). Hence, the optimum-offset processing concepts developed by Hunter et al. (1984) were adopted. The processing details can be found in Ahmad (2006); briefly, some steps worth noting include removal of the surface wave noise cone (Baker et al., 1998; Schmitt, 1999) and the refractions by a combination of top-mutes (e.g., Schmelzbach et al., 2005) and normal moveout (NMO) stretch mutes (e.g., Miller, 1992), and the use of optimum offsets. The muting unfortunately makes portions of the reflection image above ~80 ms two-way travel-time (TWT) suspect (Praeg, 2003). The length of the CMP bins was also doubled to 4 m from the nominal 2 m spacing; this doubling of the trace spacing, and hence the fold, resulted in a marked improvement in the quality of the profile. Conventional velocity analysis was carried out interactively every 50 m along the profile using the semblance method (Yilmaz, 2001).

One final, and as yet not completely satisfactorily ameliorated, problem in this study deals with lateral variations in the surface materials between mineral soil and low-velocity muskeg (sphagnum moss-filled bog). These variations result in "static" shifts to the traveltimes of reflections (see Yilmaz, 2001). In the current study, although the raw CMP gathers are of very good quality, the stacked seismic data quality deteriorated due to severe vertical and lateral velocity variations in the surface material. This makes proper normal moveout (NMO) correction difficult. Severe velocity gradients due to the presence of the near-surface water table effectively degraded the quality of the CMP (Miller and Xia, 1998). These static variations were attenuated by using a suite of methods, beginning with refraction statics based on Hagedoorn's plus-minus method (e.g., van Overmeeren, 2001). The remaining minor static errors were improved by iteratively applying surface-consistent residual statics. Regardless of these corrections, the static time shifts remain problematic and lower the quality of the profile relative to that expected from the raw shot gathers.

Resistivity Profiling
The ERT data were acquired commercially in January 2005. Cold winter conditions (<–35 °C) with deep hard snow provided good coupling of the 1 m steel electrode to the ground, making for excellent data quality. The Wenner array was used for the ERT data acquisition, using 15 m electrode spacing that would sense to depths of ~200 m. In Wenner profiling, the distance between the current and the potential electrodes remains the same, and a large number of measurements are taken in a sequence to make a "pseudosection." One potential advantage of the Wenner array is that the effect of any shallow conductive body is reduced as measurements are taken at different positions by moving the complete array along the profile.

The data were inverted using a commercially available software package Resis2dinv® (Geotomo Software, Malaysia) (Loke, 2004), which uses a nonlinear smoothness-constrained least square inversion technique (Loke and Barker, 1996) with 14 layers. A finite-element subroutine was used to calculate the forward modeling operator, a Jacobian matrix, which then was used to calculate modeled, true resistivity. As this inversion procedure is smoothness constrained, some kind of smoothing is required as an input parameter for the inversion algorithm. Moderate horizontal flatness and minimum vertical flatness were allowed during inversion.


    RESULTS
 TOP
 ABSTRACT
 INTRODUCTION
 BACKGROUND
 GEOLOGICAL BACKGROUND
 METHODS AND FIELD PROGRAM
 RESULTS
 DISCUSSION
 CONCLUSIONS
 REFERENCES CITED
 
Seismic Refraction
Long-offset, wide-angle refractions (i.e., those for which the source to receiver offset is larger than the maximum depth of investigation) were present in the data. Direct examination of the example shot gathers in Figure 5 suggests that simple layered models can be used for a first-stage interpretation (e.g., Pelton, 2005). There is a significant evolution in the shot gathers from east to west along the 10-km-long profile, and examination of these shot gathers reveals additional information about the gross structure of the valley.


Figure 05
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Figure 5. Raw common shot gathers obtained at three different vibrator points along the profile; automatic gain control (AGC) with a 150 ms averaging window has been applied to the individual traces. Various arrivals are highlighted according to the "direct" arrivals in the Quaternary fill (yellow), head wave from Paleozoic top (cyan), reflection from Paleozoic top (magenta), and head wave from top of Cretaceous (gray). The apparent velocities of the differing refracted arrivals as obtained by linear fits to segments of the first-arriving traveltimes are shown. Note the horizontal scale differences between the three panels; positive and negative offset values reflect positions of the geophones to the east and the west of the vibrator point, respectively. Highlighted green triangles represent surface wave noise cones muted from the reflection processing. (A) Easternmost shot gather over channel. (B) Shot gather at intermediate position in transition region between valley and normal sequence. (C) Western shot gather over normal bedrock. SP—shot point.

 
The easternmost shot gather (Fig. 5A) was acquired over the deepest sections of the valley that extended at least to, and in some places through, the sub-Cretaceous unconformity pK. Low-velocity, weakly consolidated Quaternary fill overlies high-velocity Paleozoic rock. The close spacing of the receivers combined with the use of geophone-singles allow the continuity of the refractions to be clearly seen. The record of Figure 5A provides a nearly classic layer-over-a-halfspace example in which the "direct" wave (yellow highlight) is associated with transit through the Quaternary fill, and the head wave (cyan highlight) arises from the top of the Paleozoic rock. One additional observation from this shot gather is the merging of the Quaternary-Paleozoic contact reflection (magenta highlight) into the direct wave. This behavior is what is expected at sufficient offsets; i.e., in the simple layer-over-a-half-space model, the reflection asymptotically approaches the direct wave. Broadly, this shot gather is consistent with two layers: the low-velocity Quaternary fill over the high-velocity Paleozoic rock.

The shot gather obtained at an intermediate position along the profile (Fig. 5B) is consistent with a two-layer model. However, while the "direct" wave (yellow highlight) is similar to that in Figure 5A and suggests propagation through Quaternary fill, the observed head wave (gray highlight) indicates both a lower-velocity and a shallower top depth that is more consistent with the Cretaceous rocks. The strong Paleozoic top reflection (magenta highlight) is still clear, but there are insufficient source-receiver offsets to observe the head wave from this interface. This shot gather still suggests a relatively thick and low-velocity Quaternary fill, but one that now immediately overlies Cretaceous siliciclastic rocks of more intermediate velocity.

The last shot gather toward the west end of the profile (Fig. 5C) is more complicated; it displays three linear arrivals that correspond to the direct wave through the Quaternary fill (yellow highlight), the head wave from the top of the Cretaceous bedrock tK (gray highlight), and the head wave from the top of the Paleozoic bedrock (cyan highlight). The strong Paleozoic reflection is still clearly seen (magenta highlight). This series of arrivals can be interpreted as a thin, low-velocity Quaternary layer that overlies a relatively thick section of moderate-velocity Cretaceous bedrock that in turn lies upon the high-velocity Paleozoic bedrocks.

Taken together, these three shot gathers illustrate the evolution of the characters of the seismic arrivals along the profile from east to west. A more quantitative, but still simple two- or three-horizontal-layer analysis was carried out using most of the shot gathers obtained in the survey in order to better understand the changes in the velocity structure along the profile. Material velocities were determined by simple linear fits to the observed traveltimes, and thicknesses were measured using the offsets and times of the crossovers (i.e., those points in the shot gathers at which different direct and head wave curves intersect). This conventional refraction interpretation gives a general idea about the subsurface structure in terms of the number of major layers, their velocities, and thicknesses. The velocity structure so determined (Fig. 6B) displays the valley as the thick, low-velocity fill immediately on top of the Paleozoic rocks to the east and the three layers of fill, Cretaceous rock, and Paleozoic rock structure outside of the valley to the west.


Figure 601
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Figure 6. (on this and following two pages). Comparison of various geophysical profiles. Profiles are all aligned and scaled the same horizontally with respect to the station number (see Fig. 1). Vertical scales all differ. (A) Time section of common midpoint (CMP) stacking velocities. (B) Depth section obtained from simple refraction analysis. (C) Apparent resistivity pseudodepth section obtained from shallow electrical resistivity tomography (ERT) profiling, logarithmic color scale.

 


Figure 602
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Figure 6. (continued). (D) Unmigrated seismic-reflection profile, grayscale with no interpretation. Compressed view of 2400 CMP at 4 m spacing. (E) Same profile as D but in color to highlight seismic amplitude variations and including some interpretive keys. Abbreviations: pK—sub-Cretaceous unconformity event, K—Cretaceous rock layering, tK—top of Cretaceous bedrock, w—washed out zones, Q1—ramp in Quaternary fill, Q2—reflective Quaternary fill, Q3—dipping features, Q4—complex reflection package at top of Paleozoic carbonates within valley, box i—expanded view in Figure 7; box ii—expanded view in Figure 8.

 


Figure 603
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Figure 6. (continued). (F) Inverted values of resistivity imaged with respect to elevation above sea level along the profile. Block parameter ization is displayed with logarithmic color ranging from 2.7 {Omega}·m to 1732.7 {Omega}·m. SC—Sousa Creek. (G) Synoptic interpretation based refraction, reflection, and resistivity profiling.

 
Seismic Reflection
The set of stacking velocities obtained in the velocity analysis (Fig. 6A) reveals the lateral changes from the low-velocity valley fill in the buried valley to the Cretaceous rock. The stacking velocities of Figure 6A are not the true material velocity but are more closely related to the root mean square average velocities, which are always lower than the true interval or material wave speeds. Despite this, the increasing velocities of the Cretaceous rock in the west are detected by this crude examination of the velocity structure and are in qualitative agreement with the refraction structure of Figure 6B.

The final seismic-reflection profile is shown in both grayscale (Fig. 6D) and in color (Fig. 6E) without and with interpretation guides, respectively. It is important to point out a number of features in the profile.

There are attenuated "washout" zones denoted by "w" in Figure 6E that extend vertically throughout the profile and in which little or no coherent reflections are observed. Such wash-outs are often observed in areas, such as shallow seafloor or lake floor sediments, with high free-gas saturation (e.g., Garcia-Gil et al., 2002).

The sub-Cretaceous unconformity at the top of the Paleozoic bedrock (pK) is the most conspicuous reflection in the profile. It is continuous across the entire line aside from the masking in washout zones. To the west of station 1400, the reflection character of pK is uniform and parallel to the weaker events above and below. Although there appears to be some minor topography on this western surface, this is more likely due to static time-shift problems. To the east of station 1400, there is a large change in the character of the pK event, which apparently begins to dip to the east. The event remains strong but is highly chaotic with much apparent topography over the range of stations from 1050 to 560 (see expanded view in Fig. 7). To the east of station 560, pK again becomes more uniform but is more reverberatory. At this location, the event also appears at greater traveltimes (>400 ms) than in the west (~375 ms).


Figure 07
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Figure 7. Expanded view of a portion of reflection profile from Figure 6E showing details of Q1 (ramp in Quaternary fill), Q2 (reflective Quaternary fill), and Q4 (complex reflection package at top of the Paleozoic carbonates within the valley) reflections at ~4:1 vertical expansion.

 
The apparent general topography of pK is mostly due to the lateral variations in the material velocities that overlie it. The lower velocities in the east (see Figs. 6A and 6B) result in a pull-down of the eastern portion of pK relative to the western section. The apparent dip between stations 1000 and 1400 is also likely indicative of a rapidly increasing thickness of the overlying lower-velocity fill material. Despite this, however, some erosion deeper into the Paleozoic section cannot be ruled out, as suggested by the sharp discontinuity in the IC sonic log (Fig. 3B) and refraction (Fig. 6B) data, and this would also contribute to the real deepening of pK.

There are a series of weaker events (K) clearly visible to the west of station 1400 that parallel pK. No evidence for these events is seen anywhere to the east of this point. These continuous events originate from the still-uneroded Cretaceous marine stratigraphy. Their disappearance to the east of station 1500, together with the traveltime pull-down effects, possibly indicates a rather steep-sided valley in agreement with the coarser refraction profile of Figure 6B. The wall of the valley, however, is not imaged. This could be due to washout of the image at this location or to difficulties encountered in imaging a steeply dipping feature in surface reflection profiles.

Q1 is an east-dipping ramp that is clearly continuous between stations 250 and 1040 and appears to represent a boundary within the Quaternary fill that delimits two seismic facies. Above Q1, Q2 marks a relatively complex package of primarily flat-lying and strong reflections above 250 ms that overlies Q1 and ranges between stations 200 and 800. This package indicates strong contrasts in the differing materials. Below Q1, Q3 highlights a series of dipping reflections between stations 1200 and1350 (Figs. 6E and 8). These are located at the transition between the valley fill and the undisturbed sediments. It is possible that the uppermost of the reflections marked Q3 could in fact be the western extension of Q1. A potential concern is that the lower events could be multiple reverberations, as examination of the full profile (Fig. 6D) in this range might suggest. However, the more detailed view (Fig. 8) shows that the two Q3 events denoted have quite different character, implying that the lower of the two is a primary reflection and not a multiple. Q4 is a complex pattern in the character of pK between CMP stations 700 and 1050. The events appear to be doubled in some parts of this zone.


Figure 08
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Figure 8. (A) Expanded view of a portion of reflection profile from Figure 6E to highlight details of Q3 (dipping features) reflections. Time is converted to depth. (B) Corresponding portion of resistivity survey from inversion of apparent resistivities of Figure 6C.

 
Resistivity Profiling
The ERT data are first shown as the observed apparent resistivities (Fig. 6C) followed by their inversion (Fig. 6F). The inversion algorithms could not avoid vertical smearing of large resistivity contrasts. Highly resistive gas-saturated zones provide one example of this smearing, and while the top of such features may be reliably estimated in the inversion, the remainder of the body cannot be resolved. A suitable color bar was selected individually for both the apparent resistivity and the final inversion to enhance all possible features along the profile, such as the conductive bedrock Cretaceous shales in the west, resistive fluvial valley in the east, and insulating potential gas-saturated zones or aquifers within the valley.

The penetration depth depends on the conductivity of the near-surface layers. The western part of section shows low resistivity, ~<15 {Omega}·m, which is due to the conductive Cretaceous shales. In the middle of the section, there is a highly resistive anomaly at ~150 {Omega}·m. This anomaly is at the western edge of Quaternary strata. The eastern part of the ERT shows low resistivity, ~15 to ~25 {Omega}·m, which could be silty clay. In the easternmost end of the profile, one higher-resistive anomaly with resistivity values of ~100 {Omega}·m is also present.


    DISCUSSION
 TOP
 ABSTRACT
 INTRODUCTION
 BACKGROUND
 GEOLOGICAL BACKGROUND
 METHODS AND FIELD PROGRAM
 RESULTS
 DISCUSSION
 CONCLUSIONS
 REFERENCES CITED
 
Taken together, both the apparent resistivities in the pseudoprofile (Fig. 6C) and the results of inversion of these data in the ERT profile (Fig. 6F) complement the seismic-refraction observations (Fig. 6B) along the 10 km extent of the profiles, where the generally resistive and lower-velocity buried valley Quaternary sediments in the east contrast with the more conductive and uneroded Cretaceous bedrocks to the west. These results are also in good agreement with the in situ log resistivities and sonic velocities (Fig. 3). Both appear to be directly underlain by the even higher-velocity Paleozoic carbonates, indicating that at this location, the valley was excavated at least to, if not through, the unconformity between Cretaceous and Paleozoic bedrocks. This gross structure is summarized in Figure 6G. Unfortunately, this single 2-D seismic and resistivity profile includes all the data available and does not allow for more informed analysis of the overall 3-D basal morphology of the valley nor of the more regional patterns and directions of buried valleys that must exist on the basis of the limited bedrock topography mapping.

Seismic-Reflection Features
The seismic-reflection profile (Figs. 6D and 6E) reveals some of the finer structure of this buried valley that may provide insight into its erosion and filling. This is discussed in terms of the various features noted here and comparisons to earlier seismic studies from Europe.

The Q4 events (Fig. 7) at the base of the Quaternary fill are complicated, and to our knowledge, similar features have not been described in previous geophysical assessments. The rough topography to pK between stations 700 and 1050 has a number of possible interpretations. First, the double reflections could be produced by 3-D structure on pK, as might be associated with motion of blocks due to glacial thrusting (e.g., Fennel et al., 2001; Rafaelsen et al., 2007) or by quarrying (e.g., Glasser and Bennett, 2004). Such deformation would likely require ice to be in direct contact with the bedrock, and it suggests that glacial abrasion was active in deepening the valley. While movement of boulders seen in glacial outwash fans by catastrophic flooding has been suggested (e.g., Brennand and Shaw, 1994; Piotrowski, 1994), the kilometer-scale continuity of the Q4 reflections argues against such a mechanism here. The two small depressions centered at common midpoint numbers 980 and 780 and bottoming near 450 ms TWT could be more local basal channels produced by subglacial or fluvial flows. However, the lack of core and transverse seismic-reflection profiles does not allow for a more informed interpretation.

Within the valley fill, the gently (<3°) eastward-dipping Q1 feature is the most continuous of the in-valley reflections, and Q1 likely represents either erosion or a change in deposition at the top of an earlier fill that has since been covered by younger materials. The dip of this event differs from the reflections both beneath and particularly above it, and this further reinforces the interpretation of a boundary, but the nature of this boundary is not known. One of Praeg's (2003) seismic images (his Fig. 4C) also shows a strong reflection dipping to the NW that is not unlike the east-dipping Q1 in Figure 7. In a similar but more controlled study, Boyce et al. (1995) showed that many of the reflections seen in their high-resolution seismic profiles correlated with erosional surfaces that separated distinct tills. Other workers (Huuse and Lykke-Andersen, 2000; Kluiving et al., 2003; Praeg, 2003) have attempted to interpret various reflections within glacial sediments on the basis of sufficiently detailed well-log information, but, to our knowledge, no study has yet been able to link a given valley-fill reflection to an actual lithological variation. One possibility is that it represents an erosional unconformity produced by glacial abrasion, and, hence, it is indicative of grounded ice and consolidation of the underlying materials. Erosion of the sediments within an already existing valley either by subglacial or surficial fluvial action is another possibility. A third possibility is rapid change in the style of deposition upon an existing surface, as evidenced by the differences in the seismic facies above and below Q1, although this change in deposition style occurs regardless of whether or not Q1 represents an erosional surface. Of these, the length (at least 3 km) and uniformity of the event suggest that the surface was produced by a uniform consolidation beneath ice.

Within the reflection profile, the eastward-dipping Q3 features are of interest (Fig. 8), and comparisons with earlier studies from the North Sea are warranted. In particular, Praeg (2003) carried out an extensive analysis of buried tunnel valleys from 2-D and 3-D seismic data over a portion of the North Sea Basin immediately to the west of the United Kingdom. Despite substantial differences in the scale and frequency content of his marine and the current land-based survey, the seismic images obtained in both are largely consistent. He noticed clinoform features within the lower portions of the valley that may be similar to the present Q3. Similar clinoform features can be seen in other marine seismic and some land seismic data sets from northern Europe (e.g., Wiederhold et al., 1998; Huuse and Lykke-Andersen, 2000; Kluiving et al., 2003), Ontario (Pugin et al., 1996), and Nova Scotia (Boyd et al., 1988). The images here (Fig. 6D) are reminiscent of these studies in that they show steep-sided valley walls, clinoform events toward the edges of the valleys, unconformities, and series of flat-lying sedimentary deposits.

The origin of such features remains controversial. Praeg (2003) argued for a time-transgressive formation of the buried valleys, which are first excavated during and backfilled during headward retreat of the margin of the ice sheet. He argued that the deeper clinoform structures are evidence of backfilling. Lonergan et al. (2006) observed series of wedge-shaped features that characterize their seismic facies unit 2. They interpreted the wedges to have been deposited subglacially and for the sediments to have come from upstream within the ice sheet, where the material consists of both eroded and reworked materials. They suggest that the on-lapping character of the reflections indicates uphill flow that would require a substantial pressure head. Kristensen et al. (2008) recently showed similar, but larger, clinoform features in marine seismic images from the North Sea. They suggested that such depositional features arise either from subglacial deposition of sediments trapped within by debris-filled ice near the toe of the glacier or from successive deltas deposited in the open valley during glacial retreat. Supercooling of the water may play a role in the development of ice and sediment trapping. The Q3 reflections highlighted in Figure 8 appear to be similar to these earlier observations, but there is insufficient supporting information to make further interpretation as to their provenance in this case.

Q2 is the package of nearly flat-lying reflections highlighted in Figure 7. The series of reflections are parallel and nearly horizontal, and this may be suggestive of glaciolacustrine deposition (e.g., Munro-Stasiuk, 2003). Such features, too, have been seen by many workers in North Sea seismic images. Lonergan et al. (2006) suggested that the subhorizontal draping package that defined their seismic facies unit 3 was deposited in quiet-water, proglacial lacustrine and latter marine settings and likely consisted of fine-grained muddy sediments. Praeg (2003), assisted in the interpretation of his "subhorizontal" seismic unit by the availability of cuttings and geophysical logs, suggested that this unit was primarily composed of lacustrine and marine muds. Earlier workers (Boyd et al., 1988; Huuse and Lykke-Andersen, 2000) suggested that these upper sections of their profiles, too, were fine-grained lacustrine sediments.

The seismic-reflection imaging highlights the complex architecture within the valley fill. Although detailed interpretations are hampered by the paucity of sufficient detail from nearby boreholes and the complete lack of any outcrop information, the reflection profile displays a number of features that are compatible with various processes related to erosion, deposition, and defor mation during multiple glacial advances and retreats, and subglacial hydrological processes. The interpretation of the gross structure of the valley is also consistent with the broad seismic interpretations of earlier workers (Boyd et al., 1988; Huuse and Lykke-Andersen, 2000; Kluiving et al., 2003; Praeg, 2003; Jørgensen and Sandersen, 2006; Lonergan et al., 2006; Kristensen et al., 2008), although these authors may disagree on finer points of valley excavation and subsequent sediment-filling processes. In other words, there does not appear to be any unique differences between the northern European structures and the one studied here, and the same processes appear to have been active at both locations.

In particular, the complexity of the structure (where the two major seismic facies are distinguished by the Q2 and Q3 seismic facies) suggests, similar to the study of Lonergan et al. (2006), that the valley here is the result of a number of processes over time. Given the depth (~350 m) of this feature and its deep bowl-like shape as mapped from well logs (Fig. 1C), it is likely that pressurized subglacial meltwater was responsible for eroding the valley. Generally, the reflections above the interpreted valley are flat-lying, suggesting that the valley-fill material was not deposited during rapid discharge events. The strong reflector that dips across the image suggests an unconformity and hence possibly indicates the existence of at least one additional erosional event. However, on the basis of the existing geophysical data alone, it is impossible to know whether this erosion occurred subglacially. The events above this unconformity are all flat-lying and suggestive of lacustrine deposition during the retreat of the glaciers.

Methane Gas
The central resistive (>100 {Omega}·m) anomaly marked "B" in Figure 6F is of particular interest because it crosses through an area where a number of wells produce economic methane from depths of only 50 m to 55 m (Fig. 1). The depth of resistivity anomaly B at 50 m closely matches with the producing horizon of those shallow wells, and, consequently, it is likely that anomaly B indicates a dry gas saturated sand.

An expanded portion of the seismic-reflection profile, converted to depth, is compared directly to the ERT data in Figure 8. The seismic image is not reliable above ~100 m depth, although close examination shows there may be some amplitude anomalies (Fig. 8A). On the ERT profile (Fig. 8B), the gas anomaly appears slightly larger than its true in situ dimensions because of the smearing effects associated with the resistivity inversion.

A detail in this study is the existence of substantial methane gas-saturated zones at shallow depths just below 30 m deep, and that this shallow gas existed in commercial quantities. The gas is clearly evident by high resistivities in the nearby electrical logs and in the ERT images. In any event, the geophysical profiles show that the gas-saturated zone lies within the glacial deposits immediately to the east of the valley edge. This is consistent with the knowledge that the gas is geochemically identical to that produced from the Cretaceous Bluesky sandstone, which was exposed by erosion of the glacial valley. It is interesting to note further that the producing gas wells (Fig. 1C) fall within an area roughly 4 km by 4 km. This suggests that there is continuity of both the porous materials and the less permeable seal material over these dimensions. However, whether these reservoirs and seals are distinct stratigraphic units over these dimensions within the valley fill is not known.

Having only a 2-D profile here, interpretations are limited, but more advanced seismic tomography algorithms could be applied to increase the lateral and vertical detail in the velocity model. This might be able to further discriminate differences in the materials above and below reflection event Q1, which is believed to originate at an erosional surface within the fill. Fully 3-D geophysical information, especially a high-resolution seismic-reflection volume, would provide additional insight into the valley detail, as shown by the numerous studies in the North Sea areas that were able to take advantage of the existence of extensive petroleum industry surveys.

As a final comment, it is worth noting that the details of the in-valley structure observed in the seismic-reflection profile cannot at present be fully appreciated because there is scant supporting geological information. It would be useful if future drilling projects were able to obtain more detailed information on the detailed stratigraphy and possibly ages of the buried valley sediments.


    CONCLUSIONS
 TOP
 ABSTRACT
 INTRODUCTION
 BACKGROUND
 GEOLOGICAL BACKGROUND
 METHODS AND FIELD PROGRAM
 RESULTS
 DISCUSSION
 CONCLUSIONS
 REFERENCES CITED
 
This study sought to provide additional information about the position, the geological setting, the internal structure, and possibly saturating fluids of a buried Quaternary valley. The well-log, seismic-reflection, seismic-refraction, and electrical resistivity tomography data provided complementary views consistent with an interpretation of a valley filled with a variety of glacial deposits. The seismic-reflection profile highlights further complexities within the valley-fill material and at the top of the eroded Paleozoic rocks that hint at various stages in the construction of the valley. However, the lack of detailed wellbore and outcrop information precludes more informed interpretation of the valley's depositional history and architecture.

This study highlights the utility of seismic and electrical geophysical investigations in delineating buried valleys. Large contrasts in compressional wave velocities and electrical resistivity between valley fill and the bounding uneroded Cretaceous and Paleozoic rocks led both the seismic and the resistivity measurements to similar interpretations of the gross valley structure. In particular, the seismic-refraction information, normally ignored in commercial surveys, provided easily obtained information that was useful to delineate the edges of the buried valley. The valley-fill structures seen in the seismic profile are similar to many of those observed in the North Sea, suggesting that they formed via similar processes.


    ACKNOWLEDGMENTS
 
In addition to the authors, the field seismic acquisition was assisted by L. Tober, M. Welz, T. He, A. Plouffe, and F. Domes. The ERT data were obtained by Komex Ltd. Seismic processing of the data was accomplished using Vista® Processing program provided by GEDCO, Calgary. We greatly thank both reviewers and the associate editor for their work in helping us to improve the paper. We also thank D. McConnell of Fugro-Jason for investigating whether acceptable airborne EM data were available for comparative purposes. Primary funding for the field programs was initiated by the Geological Survey of Canada and the Alberta Geological Survey via the Targeted Geoscience Initiative–II programs. The first author was supported through Teaching Assistantship and Research Assistantship appointments in the Department of Physics and the National Science and Engineering Research Council of Canada discovery grant to Schmitt.


    REFERENCES CITED
 TOP
 ABSTRACT
 INTRODUCTION
 BACKGROUND
 GEOLOGICAL BACKGROUND
 METHODS AND FIELD PROGRAM
 RESULTS
 DISCUSSION
 CONCLUSIONS
 REFERENCES CITED
 

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