Precipitation, landsliding, and erosion across the Olympic Mountains, Washington State, USA Stephen G. Smith, Karl W. Wegmann PII: DOI: Reference:
S0169-555X(17)30431-2 doi:10.1016/j.geomorph.2017.10.008 GEOMOR 6194
To appear in:
Geomorphology
Received date: Revised date: Accepted date:
23 January 2017 11 October 2017 12 October 2017
Please cite this article as: Smith, Stephen G., Wegmann, Karl W., Precipitation, landsliding, and erosion across the Olympic Mountains, Washington State, USA, Geomorphology (2017), doi:10.1016/j.geomorph.2017.10.008
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ACCEPTED MANUSCRIPT Precipitation, landsliding, and erosion across the Olympic Mountains, Washington State, USA
Department of Marine, Earth, and Atmospheric Sciences, North Carolina State University, Box 8208,
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a
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Stephen G. Smitha,b and Karl W. Wegmanna
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Raleigh, NC, 27695, USA b
Center for Integrative Geosciences, 354 Mansfield Road, Unit 1045, University of Connecticut, Storrs,
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CT, 06269, USA
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Corresponding author: Stephen G. Smith; email address:
[email protected]
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Abstract
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In the Olympic Mountains of Washington State, landsliding is the primary surface process by which bedrock and hillslope regolith are delivered to river networks. However, the relative importance of large earthquakes versus high magnitude precipitation events to the total volume of landslide material transported to valley bottoms remains unknown in part due to the absence of large historical earthquakes. To test the hypothesis that erosion is linked to precipitation, approximately 1000 landslides were mapped from Google Earth imagery between 1990 and 2015 along a ~15 km-wide x ~85 km-long (1250 km2) swath across the range. The volume of hillslope material moved by each slide was calculated using previously published area–volume scaling relationships, and the spatial distribution of landslide volume was compared to mean annual precipitation data acquired from the PRISM climate group for the period 1981–2010. Statistical analysis reveals a significant correlation (r = 0.55; p < .001) between total landslide volume and mean annual precipitation, with 98% of landslide volume occurring along the windward, high-precipitation side of the range during the 25-year interval. Normalized to area,
ACCEPTED MANUSCRIPT this volume yields a basin-wide erosion rate of 0.28 ± 0.11 mm yr-1, which is similar to previous timevariable estimates of erosion throughout the Olympic Mountains, including those from river sediment 10
Be, fluvial terrace incision, and thermochronometry. The lack of large historic
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yield, cosmogenic
earthquakes makes it difficult to assess the relative contributions of precipitation and seismic shaking to
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total erosion, but our results suggest that climate, and more specifically a sharp precipitation gradient,
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plays an important role in controlling erosion and landscape evolution over both short and long
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timescales across the Olympic Mountains.
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Keywords
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Olympic Mountains; Olympic Peninsula; Landslides; Erosion rates; Climate; Precipitation
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1. Introduction
The Olympic Mountains, located in the state of Washington, are situated along an active plate boundary
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in a region that receives abundant precipitation. Previous study of the Olympic Mountains has explored
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the roles of both tectonics and climate in the topographic and structural evolution of this forearc high
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(Willett, 1999; Montgomery and Greenberg, 2000; Montgomery, 2001; Montgomery and Brandon, 2002; Stolar et al., 2007), but the relative contribution of each mechanism to the surface response of the
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landscape remains unknown. The interplay among climate, tectonics, and mountain belt evolution is a research topic that has garnered much attention and debate in the 21st century (e.g. England and
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Molnar, 1990; Burbank et al., 1996; Montgomery et al., 2001; Riebe et al., 2001; Bonnet and Crave,
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2003; Whipple, 2009; Binnie et al., 2010; Korup et al., 2010; DiBiase and Whipple, 2011; Ferrier et al.,
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2013; Gasparini and Whipple, 2014), and although it is accepted that precipitation facilitates erosion in mountainous regions, deciphering the relative contribution of precipitation to overall rates and spatial patterns of erosion has proven difficult. Much of this difficulty likely arises due to complexity inherent in erosional processes across various spatial and temporal scales as well as inconsistencies in feedback cycles between climate, tectonics, and erosion across different regions of the globe. In addition to studies addressing mountain belt evolution over long (> 106 yr) timescales (e.g. Willett, 1999; Montgomery et al., 2001; Bishop, 2007; Whipple, 2009), recent research has also sought to better understand the relationship between climate and tectonics over much shorter timescales by attempting to constrain the feedbacks between rainfall, earthquakes, and erosion during and after singular meteorological or seismic events (e.g. Dadson et al., 2004; Guzzetti et al., 2004; Yanites et al., 2010; Hovius et al., 2011; Parker et al., 2011; Tang et al., 2011; Lira et al., 2013; Marc et al., 2015). These studies offer valuable information on the erosional response of particular areas to individual geologic
ACCEPTED MANUSCRIPT phenomena, but nevertheless researchers have yet to reach to reach an empirical consensus regarding
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the net effect of climate on erosion rates.
Previous studies have shown that the Olympic Mountain portion of the Cascadia forearc high is in a flux
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steady-state (Willett and Brandon, 2002) where rock exhumation, surface uplift, and erosion rates
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increase gradually from the Pacific Ocean toward the central massif and are balanced on >10 5 yr time
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scales (Brandon et al., 1998; Pazzaglia and Brandon, 2001). Over shorter timescales, less is known about patterns of erosion, with research limited to river incision and 10Be-derived catchment-averaged erosion
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rates from the Clearwater River basin (Wegmann and Pazzaglia, 2002; Belmont et al., 2007). Furthermore, since the last full-margin rupture of the Cascadia Subduction Zone occurred more than
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300 years ago (Satake et al., 1996; Yamaguchi et al., 1997), the impact of large earthquakes on the
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surface processes of individual catchments within the Olympic Mountains also remains unclear. Based
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on globally observed effects of seismic shaking in high-relief mountainous terrain, it is assumed that the AD 1700 event resulted in widespread slope failures that may have imparted a decadal-scale impact on fluvial networks and associated ecosystems (e.g. Dadson et al., 2004; Yanites et al., 2010; Hovius et al., 2011; Parker et al., 2011; Tang et al., 2011), but this assumption is unproven and it is unknown how the sediment flux from such a singular event would compare to the flux derived from, for instance, the 668 landslides inventoried in the Quinault River catchment of the Olympic Mountains during the seismically quiescent period 1939 to 1998 (Quinault Indian Nation, 1999). As a result, the relative roles of seismicity and precipitation in driving the long-term pace of erosion is a fundamental, yet unanswered question crucial for understanding mountain belt evolution and patterns of sediment flux for this and other mountain ranges in temperate, tectonically-active regions.
ACCEPTED MANUSCRIPT Here we utilize a ~1250 km2 swath across the Olympic Mountains that is oriented parallel to both tectonic (exhumation and uplift) and precipitation gradients of the range as a natural laboratory to test
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the following two hypotheses: 1) that the volume of hillslope rock and regolith displaced by landslides mimics patterns of precipitation across the range; and 2) that erosion via aseismic landsliding is a
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significant contributor to the long-term rate of erosion. We discuss our remote sensing results relative
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upland response to past climatic and/or seismic events.
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to previous research conducted within the Olympic Mountains as well as field evidence for possible
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2. Geology and climate of the Olympic Mountains
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The Olympic Mountains represent the sub-aerial portion of the accretionary wedge formed as a
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consequence of oblique subduction of the Juan de Fuca plate beneath the North American plate across the Cascadia margin. Around 15 Ma, a decrease in accommodation space led to uplift and exposure of Olympic Mountain segment of the subduction wedge above sea level (Brandon et al., 1998). At the surface, the Olympic Mountains consist primarily of the Olympic subduction complex (OSC), which is characterized by highly deformed, stratigraphically discontinuous, and partially metamorphosed sedimentary rocks (Fig. 1; Tabor and Cady, 1978; Brandon et al., 1998). Juxtaposed against the rocks of the OSC is a horseshoe-shaped surface exposure of older oceanic basalts situated on the footwall of the eastward-dipping Hurricane Ridge thrust fault (Tabor and Cady, 1978; Brandon and Calderwood, 1990; Babcock et al., 1994). These basalts, which make up the Eocene Crescent Formation (ECF), form a border along the northern, eastern, and southern sides of the range.
ACCEPTED MANUSCRIPT As the Juan de Fuca plate continues to converge with the North American plate at 36 mm yr-1, rates of uplift increase landward from ~0.3 km Myr-1 near the Pacific Coast of Washington to ~1 km Myr-1 at the
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summit of Mount Olympus, which, at an elevation of 2430 m (7980 ft), is the highest point in the Olympic Mountains (Fig. 1; Brandon et al., 1998; DeMets and Dixon, 1999). Previous research has shown
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that net uplift, or material influx into the range, is balanced by the processes of denudation, or material
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flux out of the range, and thus the Olympic Mountains currently maintain a flux steady state in which
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there is no net addition or loss of mass over geologic timescales (Pazzaglia and Brandon, 2001; Willett
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and Brandon, 2002).
The surficial geology of the Olympic Mountains is dominated by the effects of glacial and fluvial erosion
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into an uplifting massif and the formation of threshold hillslopes whose gradients are maintained by
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both shallow and deep-seated mass wasting (Montgomery, 2001). The Olympic Mountains are just
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south of the maximum extent of Cordilleran Pleistocene ice sheets, but the valleys draining the central massif were repeatedly filled with alpine glacial ice that facilitated the carving of broad U-shaped valleys with steep bedrock valley walls (Thackray, 2001; Dragovich et al., 2002). Modern alpine glaciers, which have been retreating rapidly, are restricted to the highest elevation cirque basins and to the Mount Olympus massif. Hillslope processes throughout the Olympic Mountains are dominated by bedrockinvolved landslides, debris flows, and colluvial creep down the ubiquitous steep hillslopes (Reid and Dunn, 1984; Swanson et al., 1987). Hillslope soils are rocky and thin. Shallow landslides initiating in residual soils near ridge-crests often transition into erosive debris flows that deliver sediment onto Holocene alluvial fans at the base of the steep valley sides or directly into tributary streams and axial river channels (Reneau et al., 1989; Wegmann and Pazzaglia, 2002; Benda et al., 2003). Deep-seated bedrock landslides occur both along the steep valley walls and at lower evaluations within glacio-fluviallacustrine units destabilized by post-glacial stream incision (Quinault Indian Nation, 1999; Gerstel, 1999).
ACCEPTED MANUSCRIPT At the highest elevations, gravitational spreading of steep-sided ridges (sackung) is common where sedimentary units of the OSC dip steeply towards the valley floor below (Tabor, 1971). Hillslope surficial
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geology and geomorphic processes vary little from the windward to leeward side of the range.
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Geographically, the Olympic Mountains constitute a large portion of the Olympic Peninsula and are
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unique in the United States for the combination of rugged, glacially-sculpted topography and large
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swaths of temperate rain forest (Fig. 2). Rainforest conditions exist predominantly on the western, windward side of the range due to orographic forcing as moisture-laden, land-falling Pacific storms
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encounter the steep, mountainous terrain (e.g. Minder et al., 2008; Neiman et al., 2011; Gavin and Brubaker, 2015). The bulk of precipitation, which can exceed 5 m annually in the higher-elevation
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western side of the range (Fig. 3), falls during the winter season as the Aleutian low pressure system
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intensifies and drifts south from the Gulf of Alaska, subsequently steering moisture and winds toward
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the Pacific Northwest (PRISM Climate Group, 2015; Gavin and Brubaker, 2015). While snow in lowland areas is very rare, during cold storms a significant amount of precipitation may fall as snow atop high ridges (Minder et al., 2008). Modeling of orographic precipitation patterns across the range show that deposition of snow at high elevations has a minor role in rainfall distribution, but that cold storms with low freezing levels can lead to increased leeward precipitation produced via downwind advection of frozen hydrometers generated in the orographic cloud (Zängl, 2007; Minder et al., 2008). The typically cool, rainy winters transition to warm and dry summers once the Aleutian low weakens and the North Pacific high pressure system strengthens and brings northwesterly air flow, low humidity, and sunny skies to the region (Ware and Thomson, 2000; Patterson et al., 2013).
3. Methods
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The study area encompasses a ~1250 km2 NW–SE swath across the entirety of the Olympic Mountains
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that was subdivided into a grid of 40 blocks of roughly equal area (~30 km 2) for comparison between landsliding and precipitation (Fig. 2). Within each block, individual landslides were mapped from 1990 to
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2015 using all satellite imagery available in Google Earth (Fig. 4), which included full coverage of the
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study area for the years 1990, 1994, 2005, 2006, 2009, 2011, 2012, 2013, and 2015. For the purposes of
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this study, a “landslide” consists of a large (area ≥ 5000 m2) mass movement with a well-developed rupture surface. We considered neither the failure rate nor transport distance of landslide material, as
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these factors are irrelevant to the purpose of the study. For instance, slumped material that has not been carried far from its point of origin was mapped as a complete landslide since it is now more readily
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available for transport throughout the channel network. Landslide borders were carefully drawn to
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avoid grouping multiple scars as a single unit; flow paths, chutes, and other features outside of the main
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scar were not mapped as part of the total landslide area. Potential landslides in high elevation areas with minimal-to-no vegetation were excluded from the assessment due to difficulties in identifying individual slide boundaries. Landslides affiliated with anthropogenic activity, (e.g. initiating along logging roads) were also excluded from the study. Mapped landslides were exported from Google Earth into ArcMap 10.3, where individual landslide areas and volumes were calculated, using the area-volume scaling parameters reported in Larsen et al. (2010) (Fig. 4). Based on field observations and satellite imagery, landslides with areas ≥ 5000 m2 were considered deep-seated bedrock landslides, whereas those with areas < 5000 m2 were categorized as shallow failures consisting predominately of soil and vegetation. A total landslide volume was calculated for each survey block (1–40), and volumes were normalized to block area to correct for minor differences in block size. Uncertainties in the normalized volumes include an allowed 15% mapping error for individual landslides as well as reported standard deviations (σ) for α and ϒ in the formula VL = αAϒ, where VL is landslide volume, A is landslide area, and α
ACCEPTED MANUSCRIPT and ϒ are empirically-derived constants used to estimate the volume of a landslide based on its surface area. For bedrock slides, σα = 0.03 and σϒ = 0.02, and for shallow soil slides σα = σϒ = 0.005 (Larsen et al.,
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2010). The total volume uncertainty is dependent upon the landslide size distribution within each grid block; when total volume is spread among many similarly-sized landslides, uncertainty is reduced as
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individual landslides are unlikely to be biased in the same direction, whereas when the total landslide
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less likely to be balanced (e.g., Emberson et al., 2016).
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volume of a grid block is dominated by one or several large landslides, uncertainty is high as errors are
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Grid block averages for the modeled 30-year mean annual precipitation (MAP) data (1981–2010; PRISM, 2015) were compared to total landslide volume for each block of the study area. The spatial distribution
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of precipitation is a community model output of the PRISM Climate Group, and data covering the entire
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Olympic Peninsula were obtained in ASCII format and imported to ArcMap, where MAP was averaged
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for each grid block (Figs. 2 and 3) (Table 1). The relationship between landslide volume and MAP was assessed via a linear regression model using MATLAB in which statistical significance was determined by the results of a permutation test with 107 iterations. Mean elevation and mean slope were also calculated for each grid block using the USGS 10 m digital elevation models (DEMs), and their relationship to precipitation was assessed via the same linear regression model in MATLAB.
A 25-year erosion rate for the study area was calculated by isolating landslides in the study area that occurred during the years 1990–2015 (~250 landslides; Fig. 4). These landslides were identified by viewing the 1990 imagery for each block of the study grid and progressively stepping through each later image. Any landslide that was not present in the 1990 imagery, but was identified in a later image, was included in the 25-year erosion rate calculation. The timespan between images in 1994 and 2005 requires that a landslide occurring just after the 1994 imagery still be readily identifiable 11 years later,
ACCEPTED MANUSCRIPT which is a valid assumption given that landslide scars present in the 1990 imagery persist through the most recent imagery (in 2015) used for the study. The total volume and associated erosion rates derived
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from these landslides were partitioned into “high” and “low” precipitation regions of the study area with a cutoff of 2.5 m yr-1 in which corresponding to blocks 1-18 and 20-21 receive “high” (≥ 2.5 m yr-1)
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precipitation whereas blocks 19 and 22-40 receive “low” (< 2.5 m yr-1) precipitation. We chose 2.5 m yr-1
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as the cutoff value since it corresponds to the minimum rate of precipitation received by all windward
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areas of the Olympic Mountains and allows for a simple, yet straightforward comparison of landsliding
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and erosion between the two sides of the orographic precipitation gradient.
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4. Results
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The 25-year inventory includes 937 mapped landslides that encompass an area of 4.5×106 m2 with an estimated volume of 2.0×107 m3 (Table 1). Of the 937 landslides mapped, 655 occurred in the “high” precipitation region of the study area, whereas 282 landslides occurred in the “low” precipitation region of the study area. MAP and landslide volume are significantly positively correlated (p = 0.0002; Fig. 5) via the relationship
, where the values used for landslide volume (VL(n)) have
been normalized to grid block area by dividing the total landslide volume (m3) in any given grid block by the corresponding area of that grid block (m2). In this manner, VL(n) has units of m and can be thought of as a vertical thickness of rock and regolith that is transported via landsliding in each grid block. MAP is measured as m yr-1, and the uncertainty in the slope is 1.5×10-5 ± 3.7×10-6.
Landslide volume is also positively correlated to mean slope (p = 0.008), but this correlation is mainly controlled by grid blocks 37–40 that, relative to the entire dataset, exhibit both comparatively low mean
ACCEPTED MANUSCRIPT slopes and low landslide volumes. When these grid blocks are removed, there is no correlation (p = 0.9) between landslide volume and mean slope, but landslide volume and MAP maintain a strong positive
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correlation (p = 0.002). There is no correlation between landslide volume and mean elevation (p = 0.8).
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For the years 1990–2015, total estimated landslide volume for the study area is 4.7×106 m3 (0.0047
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km3). Calculating erosion rate (Re) via the equation Re = VLA-1t-1, where VL is total landslide volume, A is
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the area considered, and t is the corresponding time interval (25 years) yields a basin-wide erosion rate of 0.15 ± 0.06 mm yr-1 (Table 2). Nearly all of this volume (98% or 4.6 x 106 m3) is derived from the
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windward, high precipitation side of the range (Fig. 6; Table 2). Calculating separate Re for high and low precipitation regions of the range via the same equation reported above results in an area-wide surface
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lowering rate of 0.28 ± 0.11 mm yr-1 for the high precipitation western flank of the range and 0.005 ±
5. Discussion
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0.002 mm yr-1 for the leeward “low precipitation” region.
Based on prior studies of post-landslide vegetation recovery (e.g. Guariguata, 1990; Smale et al., 1997; Francescato et al., 2001; Chou et al., 2009), the temperate maritime climate of the Olympic Peninsula, and observations made from satellite imagery of the study area spanning 1990–2015, we are confident that the majority of mapped landslides originally present in the 1990 imagery likely occurred during the past century, and that landslides potentially triggered by the last rupture of the Cascadia subduction zone in AD 1700 have long been revegetated and rendered mostly unidentifiable via imagery-based remote sensing techniques. As a result, we consider the volume of hillslope material moved by the mapped landslides to reflect aseismic climate-driven erosion in the Olympic Mountains, as there have
ACCEPTED MANUSCRIPT been no earthquakes large enough or in close enough proximity (c.f. Keefer, 1984) to generate coseismic landsliding on slopes of the study area during the period of seismic instrumentation (Pacific Northwest
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Seismic Network, 2016). In the absence of seismic shaking, regional landslides are the probable result of intense precipitation or rapid snow melt contributing additional moisture to wet-season near-saturated
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regolith on hillslopes, thereby decreasing the effective normal stress and leading to slope instability (e.g.
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Swanson et al., 1986; Gerstel, 1999; Quinault Indian Nation, 1999; Benda et al., 2003; Wegmann, 2004).
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The significant correlation between landslide volume and MAP supports this conclusion, as more and larger landslides are found in portions of the Olympic Mountains that receive greater amounts of rain
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and snowfall. Given that landsliding is the dominant mode of sediment transport from hillslopes to fluvial networks in mountainous environments (Hovius et al., 1997; Hovius et al., 2000; Korup et al.,
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2004; Korup et al., 2010; Wenske et al., 2012; Bennett et al., 2013), this suggests that the windward,
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wetter side of the Olympic Mountains erodes more quickly than the leeward, drier side during periods
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of seismic quiescence. This result is consistent with the pattern of long-term exhumation and rates of river incision from the range (e.g, Brandon et al., 1998; Pazzaglia and Brandon, 2001).
Calculating the 1990–2015 erosion rate from landslides allows for an assessment of climate-driven erosion with respect to long-term estimates of Olympic Mountain landscape evolution. A rate of 0.28 ± 0.11 mm yr-1 for areas of high precipitation is similar to those calculated for the Clearwater River basin using cosmogenic
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Be that integrate the catchment-averaged signal of erosion over the past 1.5 to
4×103 yrs depending on the rate associated with each individual sample (Belmont et al., 2007). This timespan includes several great earthquake events identified in paleoseismic studies focused on the CSZ (e.g. Atwater, 1987; Atwater, 1992; Atwater and Hemphill-Haley, 1997; Atwater et al., 2003; Kelsey et al., 2005; Nelson et al., 2006; Goldfinger et al., 2011; Goldfinger et al., 2012; Graehl et al., 2015), and therefore the comparable rate of modern aseismic erosion suggests that the spatial distribution of
ACCEPTED MANUSCRIPT precipitation has plays a significant role in setting the pace of late Holocene erosion. The 0.28 ± 0.11 mm yr-1 rate is also comparable to short term (annual-to-decadal) estimates of erosion based on Hoh River
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sediment yield (Nelson, 1986) as well as studies of longer-term Olympic Mountain evolution, including a ~140 ka record of river incision derived from Clearwater River strath terraces, the spatial pattern of rock
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exhumation derived from Zircon and Apatite fission track and U-Th/He thermochronology across the
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range, and estimates of erosion based on slope and mean local relief for a 10 km-wide swath across the
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Brandon, 2001; Montgomery and Brandon, 2002).
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range parallel to the Cenozoic vector of tectonic convergence (Brandon et al., 1998; Pazzaglia and
The 0.28 ± 0.11 mm yr-1 landslide-derived rate is, in fact, nearly equivalent to the mean long-term
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exhumation rate of ~0.28 mm yr-1 for the entire Olympic Peninsula (Brandon et al., 1998), which
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provides compelling evidence that climate exerts a major control on the pace of erosion. Nevertheless,
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this conclusion also raises questions about the nature of erosion on the leeward side of the range. Although every grid block assessed in this “low precipitation” portion of the range has a value of MAP that exceeds the U.S. national average (PRISM Climate Group, 2015; NOAA, 2016), aseismic landslide volume is limited and appears to have a negligible contribution to overall erosion. One possible explanation for this negligible contribution is that since slope failures in the “low precipitation zone” are not frequently triggered by local climatology and hydrology, more slopes may instead remain close to the critical threshold of stability over longer periods of time and thus fail more rapidly in the event of an earthquake as compared to slopes in the “high precipitation zone.” In this hypothesized scenario, relatively fewer landslides would occur throughout the windward side of the range since a lower percentage of slopes would be at or near the critical threshold, and thus the contribution of coseismic landslide volume to the long-term rate of erosion would be comparatively greater for the leeward side
ACCEPTED MANUSCRIPT of the range. This idea may be tested in the event of future earthquake impacts in this or other similarly
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mountainous regions having sharp precipitation gradients, such as the South Island of New Zealand.
However, confounding the above scenario is a ~0.17 mm yr-1 erosion rate derived for this study using
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sediment volume (1.56×107 m3) impounded behind the former Glines Canyon dam that was on the
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Elwha River from 1927–2012 (Bountry et al., 2011). This rate was calculated by assuming a bulk reservoir
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sediment density of 1.5 g cm-3 (e.g. Avnimelech et al., 2001; Audry et al., 2004; Snyder et al., 2004; Lazzari et al., 2015), an average rock density of 2.7 g cm-3, and dividing by the total upstream drainage
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area (632 km2) and the reservoir in-fill time (83 yrs). Although this rate is ~40% lower than our calculated rate for the windward side of the range, our hypothesis would predict a much lower rate of erosion for
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the Elwha River basin since it is located on the leeward side of the range. One explanation may be that
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climate is still an important driver of erosion for this side of the range, but that high-elevation mass
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wasting processes such as snow and debris avalanches and/or flows are the primary means of sediment release rather than landslides. We reject the possibility of anthropogenic influence because the entire Elwha River catchment above the former dam site is protected within Olympic National Park; this unexplained discrepancy is a target of future work.
Assuming the results of this study are accurate, the question of the potential impact that large earthquakes have on surface processes of upland areas, and subsequently how this manner of erosion compares to that driven by climate, still remains. Although it is impossible to quantify coseismic landsliding associated with the most recent CSZ rupture in 1700 CE, field data and observations in the upper Quinault River valley do provide evidence for possible impacts of this event. Roughly 20 km upstream of Lake Quinault, a cut-bank along the East Fork of the Quinault River exposes a massive 15 mthick, poorly-sorted unit consisting of large, angular boulders within a gravel and sand matrix. This
ACCEPTED MANUSCRIPT massive unit both overlies and is capped by ~1 m-thick beds of well-sorted fluvial gravels, a stratigraphy suggestive of disturbance in fluvial deposition caused by a large landslide event. The location of this
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deposit also corresponds with a prominent convexity in the Quinault River profile, which provides additional support for the possibility of a large, valley-blocking landslide (Fig. 7; Leithold et al., in press).
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Immediately downstream of the landslide deposit, and coincident with the confluence of Graves Creek,
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is a 5 m-high alluvial terrace that is continuous along both banks of the Quinault River for hundreds of
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meters and includes multiple buried and rooted conifer tree stumps in growth position from which limited 14C dating of outer growth rings yields a calibrated calendar age of AD 1760 ± 90 (Table 3; Fig. 7).
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This terrace deposit likely represents a relatively short period of rapid sediment accumulation that occurred as a result of breaching of the landslide dam created during the AD 1700 CSZ earthquake, after
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which the Quinault River gradually incised through the terrace and created the modern-day exposures.
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In addition to the landslide and terrace deposits at Graves Creek, the U.S. Bureau of Reclamation mapped and dated a series of well-pronounced fluvial terraces located along a ~15 km span of the Quinault River immediately upstream of Lake Quinault, with the lowest terrace yielding an age of AD 1610 ± 90 from detrital Populus charcoal and the intermediate terrace yielding an age of 1460 ± 50 cal BP from detrital conifer charcoal (Bountry et al. 2005). The age of the lower terrace, like the deposit at Graves Creek, brackets the AD 1700 CSZ earthquake and in this case suggests the possibility of channel aggradation as the result of increased sediment delivery initiated by widespread coseismic landsliding. The formation of the intermediate terrace may be similarly described, as the 1460 ± 50 cal BP age is consistent with evidence of paleoseismic sediment disruption in Lake Quinault that may have been the result of an earlier CSZ rupture or a large earthquake triggered by slip along a nearby upper crustal fault (Leithold et al., in press). Collectively, these terrace deposits indicate that seismic shaking most likely does have an appreciable impact on erosion within Olympic Mountain catchments, but that the degree
ACCEPTED MANUSCRIPT of impact may depend on both the geomorphic conditions at the time of the event (e.g., antecedent soil moisture, duration since previous event; e.g., Wegmann and Pazzaglia, 2002) as well as the degree and
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spatial extent of ground shaking produced by each earthquake, which are related to the magnitude and location of the earthquake, but are also influenced by the surrounding topography (e.g. Meunier et al.,
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2008; Buech et al., 2010; Gallen et al., 2015). This is highlighted by particularly strong evidence for
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significant Lake Quinault sediment disruption ~1500 cal BP, but limited signs of lake-wide disturbance
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resulting from any known large subsequent earthquakes (Wegmann et al., 2014; Leithold et al., in
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press).
Coupling the precipitation/landslide relationship with evidence of seismically-induced erosion suggests
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the long-term erosional evolution of the Olympic Mountains is governed in part by a balance between
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gradual, consistent climate forcing and abrupt, infrequent tectonic forcing. During times of seismic
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quiescence, areas of the range that receive abundant precipitation continue to erode at a rate comparable to the long-term average, whereas the leeward portion of the range erodes much more slowly. When large earthquakes do occur, inducing strong ground shaking, it is probable that landsliding is widespread throughout all portions of the range, but it may also be the case that landsliding is of a greater density, area, and volume in those areas that are sheltered from receiving excessive orographic precipitation. Furthermore, even the season in which a large earthquake happens may matter in terms of hillslope sediment production. For instance, if a large earthquake takes place during the winter to early spring months when slopes are saturated, the shaking may generate more hillslope failures than if the same magnitude earthquake occurred when slopes are drier, such as in August or September. We acknowledge that this hypothesis is difficult to test in the absence of seismic activity, and thus future studies should focus on developing a more complete understanding of short and long-term erosion rates for individual catchments on either side of the Olympic orographic precipitation gradient.
ACCEPTED MANUSCRIPT
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6. Conclusions
Sediment volumes calculated for mapped landslides from a ~15 km-wide swath across the Olympic
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Mountains reveal a significant positive correlation with mean annual precipitation. The windward side of
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the range, which receives abundant orographic precipitation, is characterized by a greater number of
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landslides and associated volume of transported material compared to the drier leeward side of the range. For the period 1990–2015, the total volume of landslide sediment from the windward, high-
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precipitation portion of the study area yields a mean erosion rate of 0.28 ± 0.11 mm yr -1. This rate is similar to other estimates of erosion throughout the Olympic Mountains, including those from river 10
Be, fluvial terrace incision, and thermochronometry. The similarity
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sediment yield, cosmogenic
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between our rates and those published previously suggests that climate is an important driver of both
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short and long-term landscape evolution in regions of the Olympic Mountains receiving heavy annual precipitation. Additional work is necessary to determine the precise relative contributions of climate (i.e. precipitation) and tectonics (i.e. earthquakes) to overall erosion, but our results provide compelling evidence that climate plays an important and measurable role in delivering sediment from hillslopes to the fluvial network. This has significant implications for understanding mountain belt evolution in areas with similarly sharp precipitation gradients and for comprehending the mechanisms controlling source to sink sediment fluxes in such environments.
Acknowledgements
ACCEPTED MANUSCRIPT
We thank NC State students Robert Lane, Deanna Metevier, Catherine Opalka, and Sharese Roberts for
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their assistance with landslide mapping, and to the staff of Olympic National Park for their assistance with fieldwork logistics. This work was supported in part by a Geological Society of America Graduate
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Student Research Grant and by the Geomorphology and Land Use Dynamics Program National Science
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NU
SC
Foundation (EAR-1226064).
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Table 1 Topographic, precipitation, and landslide data for each block of the study grid. mean
mean
mean annual
#
landslide
area
elevation
slope
precipitation
of
area
2
2a
(degrees)
(m yr )
landslides
(m )
1
36.5
383
20.7
3.6
12
1.81 x 10
2
30.4
568
24.0
4.0
7
3.33 x 10
3
39.2
608
25.0
4.0
20
5.63 x 10
4
41.4
622
27.5
3.7
33
3.38 x 10
5
39.5
534
24.0
3.7
13
6
16.2
698
27.0
3.8
26
7
25.8
853
26.4
4.1
23
8
40.3
877
28.2
4.2
49
9
41.6
524
27.0
3.9
10
40.0
649
26.5
3.7
11
13.3
838
28.4
4.3
12
41.5
967
28.2
4.8
13
22.4
1072
31.0
14
41.2
1183
28.3
15
41.8
638
25.0
16
38.7
1112
28.0
17
11.2
1239
18
19.9
19
40.0
MA
1.80 x 10 1.09 x 10
17
2.14 x 10
27
1.45 x 10
59
1.74 x 10
4.8
92
6.37 x 10
3.9
23
9.31 x 10
4.2
10
1.03 x 10
4.7
44
4.13 x 10
27.5
3.9
23
1.62 x 10
1095
26.4
2.9
24
1.12 x 10
1309
25.1
2.1
19
2.73x 10
AC
CE
PT ED
3.30 x 10 7.07 x 10
27.0
3.7
41
4 4 5
NU 2.04 x 10
26
1239
4
SC
(m)
40.0
landslide 3
volume
(km )
20 a
-1
landslide
PT
Block
RI
Block #
4 5 5 5 4 5 5 5 5 4 5 5 5 5
4
1.42 x 10
5
volume (m )
3 b
(m )
1990–2015
3
3
5
4
4
4
6
5
4
4
5
5
5
5
6
5
5
4
6
5
5
5
5
5
6
6
5
5
5
5
6
6
5
5
5
5
4
4
5
5
8.35 x 10 ± 3.17 x 10 1.19 x 10 ± 4.51 x 10 7.04 x 10 ± 2.67 x 10 1.94 x 10 ± 7.37 x 10 3.25 x 10 ± 1.23 x 10 9.34 x 10 ± 3.55 x 10 3.93 x 10 ± 1.50 x 10 1.98 x 10 ± 7.54 x 10 1.47 x 10 ± 5.57 x 10 1.84 x 10 ± 6.98 x 10 5.54 x 10 ± 2.10 x 10 3.86 x 10 ± 1.47 x 10 3.25 x 10 ± 1.24 x 10 2.90 x 10 ± 1.10 x 10 4.97 x 10 ± 1.89 x 10 2.83 x 10 ± 1.08 x 10 7.01 x 10 ± 2.66 x 10 3.44 x 10 ± 1.31 x 10
3
3
5
4
4
4
5
5
4
4
5
4
5
5
4
4
4
4
4
4
5
5
5
4
6
5
2
1
5
4
5
5
5
4
5
4
6.22 x 10 ± 2.36 x 10 1.15 x 10 ± 4.36 x 10 6.97 x 10 ± 2.65 x 10 7.92 x 10 ± 3.01 x 10 2.75 x 10 ± 1.04 x 10 2.12 x 10 ± 8.07 x 10 3.29 x 10 ± 1.25 x 10 6.03 x 10 ± 2.29 x 10 6.73 x 10 ± 2.56 x 10 8.51 x 10 ± 3.23 x 10 3.55 x 10 ± 1.35 x 10 1.80 x 10 ± 6.84 x 10 1.41 x 10 ± 5.37 x 10 1.17 x 10 ± 4.45 x 10 1.34 x 10 ± 5.08 x 10 3.67 x 10 ± 1.40 x 10 1.42 x 10 ± 5.40 x 10 2.30 x 10 ± 8.72 x 10
3.43 x 10 ± 1.30 x 10 3.71 x 10 ± 1.41 x 10
0 3
4.68 x 10 ± 1.78 x 10
3
A 15% error is assumed for the mapping procedure.
b
Uncertainty includes propagated errors from the determination of landslide area and standard deviation for α and ϒ in the formula, V = αAϒ, used to calculate landslide volume (VL).
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Table 1 (continued) Topographic, precipitation, and landslide data for each block of the study grid.
2
(m)
(degrees)
mean annual precipitation -1 (m yr )
# of
landslide area
landslides
(m )
5
35.7
1253
28.1
2.9
86
2.08 x 10
22
9.3
1070
25.4
2.4
46
1.19 x 10
23
38.1
1449
26.9
1.9
14
4.41 x 10
24
26.5
1541
26.6
2.0
4
25
41.4
985
29.6
2.1
19
26
39.5
995
25.5
1.9
22
27
33.3
1640
26.5
1.9
12
28
22.8
1669
27.2
1.9
16
33 34 35
24.1 22.1 23.0 24.0
1477 1310 1256 1444 1020
27.6 28.6 28.9 28.3 26.8 25.3
1.2
13 2 4
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3.52x 10
2.19 x 10 1.16 x 10 2.64 x 10 5.83 x 10 1.14 x 10
2.84 x 10
728
13.2
1.2
12
6.71 x 10
489
15.6
1.0
10
1.76 x 10
714
38
39.5
39
41.8
435 n/a 1010
15.3 n/a 25.7
1.0 n/a 2.8
3 937 23.4
5 4 4 5 4 4 4 4
4
2
42.2
29.8
1.6
27
1.22 x 10
1.2
37
AVERAGE
1.3
37
5.75 x 10
17.7
23.6
1258
1.5
8
2.83 x 10
2.61 x 10
741
SUM
1.8
2
8.17 x 10
10
34.6
18.4
1.8
1.02 x 10
1.2
36
40
1.8
2.53 x 10
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32
25.1
1545
30.4
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31
32.3
1619
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30
22.8
landslide volume
2a
21
29
a
mean slope
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(km )
mean elevation
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Block area
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Block #
7.73 x 10
5 5 4 3 4 4 3 3 4 3
4.53 x 10
6
landslide 3 volume (m )
3 b
(m )
1990–2015
5
5
5
4
5
4
4
4
5
5
5
4
4
4
5
4
4
4
5
4
5
5
5
5
4
3
3
3
4
4
4
4
3
2
3
3
3
3
3
3
7
6
5
5
5.39 x 10 ± 2.05 x 10 2.37 x 10 ± 8.99 x 10 1.52 x 10 ± 5.77 x 10 9.99 x 10 ± 3.79 x 10 3.48 x 10 ± 1.32 x 10 2.50 x 10 ± 9.48 x 10 5.91 x 10 ± 2.25 x 10
3
3
3
3
2
1
2
2
3
2
2
2
2
2
4.05 x 10 ± 1.54 x 10 7.95 x 10 ± 3.02 x 10 2.37 x 10 ± 9.01 x 10 2.67 x 10 ± 1.01 x 10 1.76 x 10 ± 6.67 x 10 7.01 x 10 ± 2.66 x 10 3.56 x 10 ± 1.35 x 10
1.49 x 10 ± 5.67 x 10
0
4.84 x 10 ± 1.84 x 10
0
1.14 x 10 ± 4.32 x 10
0
8.85 x 10 ± 3.36 x 10
0
4.95 x 10 ± 1.88 x 10
0
1.28 x 10 ± 4.88 x 10
0
2.89 x 10 ± 1.10 x 10
0
2.66 x 10 ± 1.01 x 10 6.85 x 10 ± 2.60 x 10 1.29 x 10 ± 4.91 x 10 2.76 x 10 ± 1.05 x 10
0 4
4
2
2
2
1
6.27 x 10 ± 2.38 x 10 2.72 x 10 ± 1.04 x 10 2.15 x 10 ± 8.15 x 10
8.25 x 10 ± 3.13 x 10
0
3.83 x 10 ± 1.46 x 10
2.02 x 10 ± 7.69 x 10 5.06 x 10 ± 1.92 x 10
0 6
6
5
4
4.67 x 10 ± 1.77 x 10 1.17 x 10 ± 4.43 x 10
A 15% error is assumed for the mapping procedure.
b
Uncertainty includes propagated errors from the determination of landslide area and standard deviation for α and ϒ in the formula, V = αAϒ, used to calculate landslide volume (VL).
ACCEPTED MANUSCRIPT Table 2 Landslide volumes and erosion rates for high and low precipitation areas of the study region. Area
region
2
elevation
Mean slope
mean
landslide
precip
volume (m )
rate
-1
(mm yr )
(m)
(degrees)
(m yr )
1990–2015
4.60 x 10 ± 1.75 x 10
657
848
27.0
3.93
Low Precipitation (leeward)
601
1172
24.7
1.63
7.45 x 10 ± 2.83 x 10
All
1258
1010
25.7
4.67 x 10 ± 1.77 x 10
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High Precipitation (windward)
2.78
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a
erosion
3 a
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(km )
Mean
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Study
-1 a
6
6
0.280 ± 0.106
4
4
0.005 ± 0.002
6
6
0.149 ± 0.056
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Uncertainty includes propagated error from landslide area and 1σ standard deviation for α and ϒ in the formula, VL ϒ = αA , for landslide volume (VL).
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Table 3 Radiocarbon (14C) geochronology data for East Fork Quinault River landslide deposit.
(‰)a
%MC
-22.5
97.31
Radiocarbon age
1 error 0.33
BP 219
1 error 27
Calibrated ageb
cal AD range
probability
1640–1685 1735–1805 1935–
37.20% 44.50% 13.70%
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D-AMS 007634
Fraction of modern
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Lab ID
(13C)
All results have been corrected for isotopic fractionation with 13C values measured on the prepared graphite using the AMS spectrometer
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a
b
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Radiocarbon calibration was performed using the OxCal 4.2 online calculator using the IntCal 13 calibration curve (Bronk Ramsey, 2009). Results were rounded by 5 years.
ACCEPTED MANUSCRIPT Figures (if not included as separate file) and Figure Captions
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Fig. 1. Geologic setting of the study area. Top Inset: Simplified tectonic map of the Cascadia subduction zone. The Olympic Mountains (OM) study area is outlined by the dashed box. Main map: Simplified
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geologic map of the Olympic Peninsula (from Dragovich et al. 2002) draped over a hillshade of digital topography. Sedimentary rocks of the Olympic Subduction complex (OSC) are in green, while basalts of
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the Eocene Crescent Formation (CF) are colored in brown. Faults are shown by solid or dashed (inferred) black lines. The Hurricane Ridge fault (HRF) marks the contact between the OSC and peripheral rocks
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such as the CF. Faults with Holocene surface rupture are as follows: Seattle fault zone (SFZ); Saddle Mountain fault zone (SMFZ); Canyon River fault (CRF); Hood Canal fault (HCF); Tacoma fault zone (TFZ);
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and Lake Creek – Boundary Creek fault (LC-BCF). The black-lined polygon delineates the study area
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swath.
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Fig. 2. Study area outlined on a satellite image of Washington’s Olympic Peninsula. The locations of Mount Olympus, Lake Crescent, Lake Quinault, the Clearwater River basin, the Glines Canyon dam,
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Graves Creek, and the downstream reaches of major rivers (white lines) are provided for regional context and also for references made in the discussion section of this paper. The study area swath is delineated by the white-lined polygon consisting of 40 numbered grid blocks. Boundaries of individual grid blocks are based on Public Land Survey Township and Range subdivisions for western Washington State; the average block area is 31 km2.
Fig. 3. Precipitation distribution in the study area. Left: Distribution of mean annual precipitation (MAP; cm yr-1) for the period 1981–2010 draped over hillshaded digital topography of the Olympic Peninsula (PRISM, 2015). The study area is outlined in black and downstream reaches of major rivers are identified and labeled. Right: Precipitation and elevation profiles across the Olympic Mountains from A to A’ (see the left panel for location). Note the abrupt decrease in precipitation to the east of km ~60 that separates the western windward from the eastern leeward sides of the range.
ACCEPTED MANUSCRIPT Fig. 4. Google Earth images of landslides. A: Perspective-view example of delineated landslides within the Upper Quinault River catchment using Landsat imagery available in Google Earth (grid block 13). B: Area calculations derived by importing the landslide polygons originally determined in Google Earth into
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ArcMap 10.3. In the lowest-elevation polygon, landslide volume is written in red font below the surface area determination. Volumes were calculated using power-law scaling parameters reported in Larsen et
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al. (2010). C and D: Perspective-view example of a post-1990 landslide utilized for erosion rate
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calculation. C shows Imagery from 1990 with scar of future landslide outlined by the white dashed line. D shows post-landslide imagery from 2013 with the same white dashed line delineating the landslide. The depicted landslide occurred along Rustler Creek in the North Fork Quinault River catchment (grid
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block 13). Coordinates for the centroid of each photo are as follows: A/B: 47.6739° N, 123.6204° W; C/D:
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47.6358° N, 123.5958° W.
Fig. 5. Plot of area–normalized landslide volume (VL(n); m) versus mean annual precipitation (MAP; m yr1
) for each of the 40 blocks within the study grid. Vertical error bars represent propagated uncertainty in
the volume calculation (see Methods section for details). The equation, VL(n) = 1.5×10-5MAP, represents the significant positive relationship between MAP and VL(n) (p = 0.0002) as determined using a permutation test.
Fig. 6. Relative contribution of high-precipitation (grid blocks 1–18 and 20–21) and low-precipitation (grid blocks 19 and 22−40) areas to total landslide volume for the period 1990–2015. The study area (including the division between “high” and “low” areas of precipitation) is outlined in black, and
ACCEPTED MANUSCRIPT downstream reaches of major rivers are marked with black lines. Over the 25-year span, 98% of landslide volume has been produced in the high precipitation, windward portion of the study grid,
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yielding an erosion rate of 0.28 ± 0.11 mm yr-1 for this area.
ACCEPTED MANUSCRIPT Fig. 7. Field and geochronological evidence for the impact of the AD 1700 Cascadia subduction zone earthquake on the upper Quinault River catchment. A: Contour map of the area surrounding the confluence of Graves Creek and the East Fork of the Quinault River (see arrow on Fig. 2 for location).
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Hypothesized valley-blocking landslide is mapped in yellow and downstream event terrace is mapped in orange; consult discussion for additional details. Black star corresponds to the location of (C); white star
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corresponds to the location of (D). B: Panoramic photograph of the northern cut-bank of the Quinault
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River, just upstream of the confluence with Graves Creek. The 5 m-thick event terrace is visible on the downstream (left) side of the image and a portion of the 15 m-thick landslide deposit is visible on the right, upstream side of the photo. C: Photograph of the 15 m-thick landslide deposit; the boulder
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outlined in white has a long axis of approximately 1 m. D: Photograph of the event terrace from the opposite bank of the Quinault River, just downstream of Graves Creek. The blue star indicates the
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location of the 14C sample acquired from the outermost growth rings of one of several large trees buried in place by the aggradation of sediment now recorded as the event terrace upon which a mature conifer
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forest is now growing.
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ACCEPTED MANUSCRIPT Highlights
Landslide volume is positively correlated with mean annual precipitation.
A calculated basin-wide erosion rate of 0.28 ± 0.11 mm yr-1 is consistent with previous research.
Between 1990-2015, 98% of landslide volume occurred in areas of high precipitation.
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1.1
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1.2