The impact of over 100 years of wildfires on mercury levels and accumulation rates in two lakes in southern California, USA
In southern California, USA, wildfires may be an important source of mercury (Hg) to local watersheds. Hg levels and Hg accumulation rates were investigated in dated sediment cores from two southern California lakes, Big Bear Lake and Crystal Lake, located approximately 40-km apart. Between 1895 and 2006, fires were routinely minimized or suppressed around Big Bear Lake, while fires regularly subsumed the forest surrounding Crystal Lake. Mean Hg concentrations and mean Hg accumulation rates were significantly higher in Crystal Lake sediments compared to Big Bear Lake sediments (Hg levels: Crystal Lake 220 ± 93 ng g−1, Big Bear Lake 92 ± 26 ng g−1; Hg accumulation: Crystal Lake 790 ± 1,200 μg m−2 year−1, Big Bear 240 ± 54 μg m−2 year−1). In Crystal Lake, the ratio between post-1965 and pre-1865 Hg concentrations was 1.1, and several spikes in Hg levels occurred between 1910 and 1985. Given the remote location of the lake, the proximity of fires, and the lack of point sources within the region, these results suggested wildfires (rather than industrial sources) were a continuous source of Hg to Crystal Lake over the last 150 years.
KeywordsMercury California Wildfires Rapidly deposited layers Turbidites
Mercury (Hg) is a naturally occurring element in the Earth’s crust, which may be liberated through natural or anthropogenic means. Once released Hg may be transformed into methylmercury (MeHg), which is efficiently biomagnified in the aquatic food web. In the troposphere, Hg exists as gaseous elemental Hg (Hgo), reactive gaseous mercury (RGM, consisting of oxidized gaseous Hg(II) compounds), or Hg may be bound to particulates (Hgp) (Lindberg et al. 2007). RGM and Hgp have relatively short atmospheric residence times and may be deposited within hours to weeks, while the tropospheric residence time for Hgo is between 6 months and 2 years (Schroeder and Munthe 1998).
Wildfires and biomass burning are significant sources of Hg emissions to the atmosphere (Brunke et al. 2001; Engle et al. 2006; Friedli et al. 2001, 2003a, b; Harden et al. 2004; Veiga et al. 1994; Wiedinmyer and Friedli 2007). During a wildfire, Hg is primarily emitted from vegetation and soils in the form of Hgo. In a smoke plume, most Hg (>87%) is in the form of Hgo, while the remaining is bound to particulates (Hgp); however, the ratio between the two is fuel-dependent (Friedli et al. 2003a, b). Although Hg is released primarily as Hgo, increased MeHg levels have been observed in the vicinity following a wildfire. Caldwell et al. (2000) reported sediment MeHg levels peaked within 3 months after a wildfire (64-km downwind from the fire origin) due to increased storm runoff and transport of Hg and MeHg, while Amirbahman et al. (2004) observed elevated MeHg levels in soils burned 45 years prior to Hg analysis, indicating soil changes following a fire (e.g., higher soil pH) persisted for years. Fires also enhance productivity in lakes through deposition of nutrients (Spencer et al. 2003), which may increase MeHg levels in fish tissue by lengthening the food chain (Kelly et al. 2006), or nutrients may decrease MeHg biomagnification in fish tissue due to algal bloom dilution (Chen and Folt 2005; Pickhardt et al. 2005).
In southern California, March to October is considered the fire season; however, the length of the season is dependent on winter precipitation levels. A number of water bodies in this region are listed as impaired for Hg in water, sediments and/or fish tissue (USEPA 2008), although there are no coal burning power plants and few other atmospheric point sources of Hg within the air shed. In this semi-arid region, fires may be a significant source of Hg. Forest fires produce ash, which may contain heavy metals that are easily solubilized and may impair water quality (Plumlee et al. 2007). Soils coated with ash are more water repellent than unburned sediments, causing increased erosion and higher runoff (Onda et al. 2008; Shakesby and Doerr 2006). While the effect of fires on lake sedimentation and water chemistry has been well documented (Gresswell 1999; Malmon et al. 2007; Minshall et al. 1989; Spencer et al. 2003), the impact of wildfires on historical sediment Hg levels has not previously been investigated.
Site descriptions and fire history
Big Bear Lake, CA
Big Bear Lake (elevation: 2,055 m) is located in the San Bernardino Mountains in the Santa Ana watershed (34.24° N, 116.90° W). Lake levels are primarily dependent on precipitation (rain, snow) and evaporative processes. The surface area of the lake is 12 km2 and the watershed is 140 km2 (USDANRCS 1999). Average depth of Big Bear Lake is 7.3 m, although near the dam the depth ranges from 15 to 22 m. Big Bear Lake is moderately eutrophic, and during the summer months may exhibit severe oxygen depletion at depth (Siegfried et al. 1982). Big Bear Lake was first included on California’s List of Water Quality Limited Segments for Hg in 1998 due to Hg levels >0.3 ppm in fish tissue (USEPA 2008), the recommended level for safe consumption (USEPA 2001).
List of fires that burned more than 25 km2 and were <10 km from each lake, 1895–2006
Name of fire
Area burned (km2)
a Big Bear Lake
51 additional fires that burned <25 km2
Total area burned <10 km from Big Bear Lake, 1895–2006
b Crystal Lake
38 additional fires that burned <25 km2
Total area burned <10 km from Crystal Lake, 1895–2006
Crystal Lake, CA
Crystal Lake (elevation: 1,657 m) is located within the Angeles National Forest at the headwaters of the San Gabriel River watershed (34.19° N, 117.50° W), and is fed by primarily small springs and precipitation (rain, snow). Lake level is controlled by precipitation and evaporation. Several recently incised gullies revealed organic-rich, fine-grained sediment, which may reflect past periods of sustained high lake levels. A well-defined tree line delineates the average historical high lake level position, which was substantially higher than the modern lake level. A recently felled tree near the tree line contains 160 rings, which provides a possible minimum age for the last episode of sustained lake level above the tree line. Aside from one event in the late 1800s when Crystal Lake was drained for agricultural purposes and then refilled (Conrad 2003), lake levels were not recorded.
Limnologically, the lake undergoes strong seasonal stratification and bottom water anoxia (depth ~7 m). Crystal Lake’s surface area is <0.023 km2 and the immediate drainage basin surrounding the lake is quite small (~0.50 km2). Crystal Lake was first included on California’s List of Water Quality Limited Segments in 1996 for organic enrichment and low dissolved oxygen (USEPA 2008), but was not listed as impaired for Hg. Although recreational fishing is a beneficial use for Crystal Lake (LARWQCB 1994), Hg levels in fish tissue are not monitored, most likely due to the relatively few number of visitors to the lake compared to other recreational sites (e.g., Big Bear Lake).
Unlike Big Bear Lake, which is populated by homes and small businesses, the immediate vicinity of Crystal Lake is surrounded by pine forest, and fires frequently engulf the area around Crystal Lake (Fig. 2b). Between 1895 and 2006, fires charred 1,160 km2 within 10 km from Crystal Lake (1.9 times the area burned neared Big Bear Lake) (USDAFS 2008). Compared to Big Bear Lake, more frequent, larger fires (>25 km2) occurred within 10 km of the lake (11 vs. 2) (Table 1). Of these 11 fires, severe fires (>80 km2) occurred in 1919 (East Fork San Gabriel River Fire), 1924 (San Gabriel Fire), 1957 (Gale Fire), and in 2002 (Curve Fire and Williams Fire; Fig. 2b; USDAFS 2008).
Length (cm) and location for all sediment cores from Big Bear Lake and Crystal Lake, the method used for Hg analysis (EPA 7473 or EPA 1631), the mean and range in Hg levels (ng g−1), and sample size (n)
Mean (ng g−1)
Range (ng g−1)
Big Bear Lake
N 34° 14.42′
W 116° 57.56′
N 34° 14.60′
W 116° 55.09′
N 34° 19.11′
W 117° 50.84′
N 34° 19.10′
W 117° 50.83′
N 34° 19.12′
W 117° 50.83′
Big Bear Lake, CA
Two cores, BBL-GC-2003-1, (52 cm, hereafter referred to as BBL-1) and BBL-GC-2002-2 (34 cm, hereafter referred to as BBL-2) were extracted from the western side of Big Bear Lake near the dam, the former in November 2003 and the latter in 2002. BBL-1 water depth was 11 m, and BBL-2 water depth was 13 m. BBL-2 sediments were freeze-dried, while BBL-1 sediments were archived in cold storage (4°C). Analysis of Hg levels was completed in 2004 for the BBL-2 and in 2007 for BBL-1.
Crystal Lake, CA
In 2003, sediment cores were extracted from the lake’s deepest basin (6.4 m), near three active gullies. Three cores (CL-PC-2003-01, CL-GC-2003-02, and CL-GC-2003-04 hereafter referred to as CL-1, CL-2 and CL-4, respectively) were opened, visually described and then archived in cold storage (4°C) (Table 2). Hg was analyzed in CL-1 and CL-2 sediments in 2007, and CL-1 was re-analyzed in 2009. CL-4 is included in this analysis for illustrating the coherent stratigraphy across the lake basin.
Except for core BBL-2, storage, splitting and slicing of sediment cores, as well as measurement of loss-on-ignition 550°C and 950°C, grain size analysis, and selection of material for dating was completed at the Cal State Fullerton Paleoclimatology Lab (CA, USA). Core BBL-2 was sectioned and freeze-dried at the University of Southern California (CA, USA). Hg analysis for BBL-1, BBL-2, CL-1 (using EPA 7473), and CL-2 was completed at the University of California, Los Angeles (CA, USA), and Hg analysis of CL-1 (using EPA 1631) was completed at the State Key Laboratory of Environmental Geochemistry (Guiyang, China).
Solid-phase Hg levels were determined in sediment slices using two methods: EPA Method 7473 (USEPA 1998) and EPA Method 1631 (USEPA 2002). Core BBL-2 was analyzed using EPA Method 1631, BBL-1 and CL-2 were analyzed using EPA Method 7473, and CL-1 was analyzed using both methods (Table 2). For both methods, standard trace metal protocols were followed.
Approximately 1 g of sediment was digested in acid-cleaned vials overnight in 10 ml of either 8:2 or 3:1 hydrochloric acid:nitric acid. Samples were oxidized with bromine monochloride, and excess oxidant was neutralized with hydroxylamine hydrochloride. Samples were further reduced with stannous chloride, converting Hg(II) to the more volatile Hgo, which was purged from solution by argon gas. Quantification was by dual-stage gold amalgamation/cold vapor atomic fluorescence spectrometry (CVAFS). The oxidation–reduction steps follow established methods (Bloom and Crecelius 1983; Bloom and Fitzgerald 1988).
Sediments were measured using direct Hg analysis by thermal decomposition, amalgamation, and atomic absorption spectrophotometry. No pre-analysis steps were required.
Hg resolution and QA/QC
Hg was analyzed in 1-cm contiguous slices in core CL-1 using EPA 1631 and every 2–5 cm using EPA 7473 (Table 2). For the remainder of the paper, results from the former method were discussed, since more strata were analyzed and the correlation between Hg levels using the two methods was 0.78 (n = 17). For BBL-1 and BBL-2, a 1–2 cm interval was analyzed, while every 2 cm were analyzed within CL-2 (Table 2).
The method detection level (MDL) was measured using t*standard deviation of method blanks, where t represented the level for specific n at which there is <1% chance of a Type 1 error, i.e., including a sample not significantly different from 0 (40 CFR, Appendix B to Part 136). For Method 1631 the MDL was 4.2 ng g−1 (n = 6, t = 3.365) and for Method 7473 the MDL was 4.7 ng g−1 (n = 8, t = 2.998). MDLs for both methods were higher than values typically reported, most likely due to variability in Hg levels in beach sand (used as the matrix blank), which increased the standard deviation. For both methods, all measured Hg values in the sediment cores were greater than the MDL.
Recovery of standard reference material (IAEA-405 estuarine sediment, IAEA-433 marine sediment, GBW-07405) was 100 ± 3.3% (n = 26) for EPA 7473, and for EPA 1631 recovery averaged 104 ± 8.3% (n = 8). For BBL-1 (EPA 1631), BBL-2 (EPA 1631), CL-2 (EPA 7473), and CL-1 (EPA 7473 only) all sediment slices for Hg were analyzed in triplicate. Reproducibility was measured using relative standard deviation (RSD, 100 × sd/mean) between triplicate measurements. For EPA 7473, RSD averaged 13 ± 13% (n = 64) and for EPA 1631 RSD averaged 2.4 ± 1.6% (n = 33). A subset of CL-1 sediment slices (analyzed by EPA 1631) was measured in duplicate, and the relative percent difference (RPD) averaged 15 ± 12% (n = 6).
Wet sediments were dried overnight in a 60°C oven using pre-weighted crucibles, and the wet:dry ratio of the sample was determined. Hg concentrations are reported on a dry weight basis.
All sedimentological parameters were analyzed at 1-cm contiguous intervals.
Mass magnetic susceptibility
Mass magnetic susceptibility is a measure of the iron (Fe)-bearing minerals within sediments, predominantly Fe oxides. Sediment samples were placed in 8-cm3 plastic cubes, and mass magnetic susceptibility was measured twice on each sample with the y-axis rotated 180° once per analysis, using a Bartington MS2 Magnetic Susceptibility instrument at 0.465 kHz. All magnetic susceptibility data were determined within 24 h of splitting the core in order to minimize oxidation effects.
Loss-on-ignition 550° and 950°C
Samples were combusted for 2 h at 550°C (total organic matter) and for an additional 2 h at 950°C (total carbonate); loss-on-ignition (LOI) was calculated after each heating (Dean 1974). For total carbonate, values <3–4% may reflect clay de-watering, and hence were interpreted as 0% (Dean 1974).
Analyses of microfossils (oogonia, the reproductive capsule of Chara) and charcoal were completed for Crystal Lake (CL-1). Prior to microfossil analyses, sediments (2–5 g) were disaggregated using 10% sodium hexametaphosphate. After 1–3 days, sediments were sieved (250 μm), and remaining sediment was filtered, air-dried, and weighed. The sediments were split as required to reduce the total specimens for analysis. Using a standard binocular microscope, the number of charcoal pieces and oogonia were counted, corrected for splits and then normalized to the total number of specimens per 5 g of dry sediment.
Bulk density was determined by measuring the mass of wet or dry sediment in a known volume. For wet sediments, bulk density was converted to dry mass using percent water.
Grain size analysis
Grain size analysis was determined for cores BBL-1 and CL-1. Prior to grain size analysis, detrital material >2,000 μm was removed by wet sieving, and organic matter was volatilized using successive additions of 30% hydrogen peroxide (H2O2) until no reaction occurred. Sands were split to achieve a desired obscuration of 3–5%; clays and silts were split to achieve an obscuration of 8–14%. Instrument accuracy and precision were verified daily and for every 10 samples using a tuff standard (TS2) with a known distribution between 1.00 and 16.0 (average 4.53 μm ± 0.07; n = 2,998). Two separate standard operating procedures were used for sands and clays/silts, both based on the Mie Scattering principle. Size distributions are reported as volume percent clay (0.02 μm to 3.89 μm), silt (3.90 μm to 73.9 μm), and sand (74.0 μm to 2,000 μm).
For core BBL-1, bulk elemental composition was determined on 17 samples using a Phillips PW 2400 X-Ray Fluorescence (XRF) scanner at UC Berkeley (lead, zinc, iron, chromium, copper, nickel, vanadium, and aluminum). Samples were dried, ground, treated with a bonding agent, and compressed into pellets.
Age control for Big Bear (BBL-1) and Crystal Lake (CL-1) cores was determined using (1) surface sediment age based on an intact sediment–water interface (BBL-1 and CL-1), (2) 137Cs analyses (BBL-1 and CL-1), (3) elemental Pb concentrations (core BBL-1 only), and (4) 210Pb analyses (core CL-1 only). Analysis for 210Pb is used to date young (<200 year) sediments (Appleby and Oldfield 1978; Crusius and Anderson 1995; Krishnaswami et al. 1971), while 137Cs is used to determine the year (1963) for maximum nuclear fallout from weapons testing (Robbins and Edgington 1975), as well as the year when 137Cs first appeared in measurable levels in environmental samples (1954) (Ritchie and McHenry 1990). For 137Cs, 2–6 g of sediment were sealed in 60 × 15 mm plastic petri dishes, aged for 30 days and counted on a gamma spectrometer (Hyperpure Ge detector) for the determination of 137Cs and 226Ra. 226Ra was also analyzed on selected slices by the radon de-emanation technique (Mathieu 1997; Wilkinson 1985). For 210Pb, 1-g samples were leached in 6 N HCl in the presence of a 209Po. Po was autoplated onto a silver disc (Flynn 1968) and counted on an alpha spectrometer to determine 210Pb via its 210Po daughter, and excess 210Pb was determined in each slice by subtracting the 226Ra activity. For core BBL-1, a peak in elemental Pb, measured using XRF (described in “Sedimentology”), was used as an age based on the removal of lead from gasoline in the 1970s (1975 ± 5 year) (Callender and Rice 2000).
Hg accumulation rates
Results and discussion
Core descriptions and age control
Big Bear Lake
BBL-1 surface sediments were dated as 2003, the year the core was extracted (see Fig. 3d); a peak in elemental Pb at 30 cm was assigned an age of 1975 ± 5 year; a peak in 137Cs at 31 cm was assigned the date 1963; between 45 cm and the base of the core, 137Cs was no longer measurable and represented sediment deposited before 1954; the bottom of the core (50 cm) was inferred as ~1950 s ± 5 year, corresponding to a decrease in lake level. Between 1946 and 1951, lake level recorded near the dam decreased from 19 to 10 m, the lowest level recorded since 1904, which was due to a prolonged period of below average precipitation levels (~20 year) and heavy irrigation demands (BBMWD 2008). Between 1951 and 1961, lake level averaged 13 m. In the 1960s, lake level increased from 10 to 21 m, and between 1969 and 2004 lake level averaged 19 m. The basal age for core BBL-1 (~1950s ± 5 year) was based on a sharp increase in sand (from 9.0% to 82%), which represented an encroachment of the littoral zone into the deep basin during the low stand, or the rapid influx of sediment as lake level rose following the low stand (Fig. 3c). Likewise, the bottom of BBL-2 (34 cm) was assigned a date of 1950s ± 5 years due to the steep increase in sand, similar to core BBL-1. In 1964 the Big Bear Water District was formed to regulate water dissemination from the lake, and in 1977 irrigation withdraws were halted (BBMWD 2008).
Core CL-1 was dominated throughout by a silty sand except from 2 to 7 cm and 57 cm to 69 cm, where sand was the dominant grain size. On average, clay accounted for 7.7% of the grain size distribution, while silt and sand accounted for 54% and 38% of the distribution, respectively. The sediment color was highly varied from light gray to dark brown; the core section between 14 and 38 cm was characterized by faint laminations.
For core CL-1, the age of the intact sediment–water interface was assumed to be 2003, when the core was extracted. A peak in 137Cs occurred at 20.5 cm and was assigned 1963 (Fig. 4d). Using 210Pb values, the depth–age profile was calculated using the constant rate of supply (CRS, Appleby and Oldfield 1978; Appleby 2001). The CRS model assumes the sediment transport parameters are independent of the sedimentation rate and there is a constant influx of unsupported 210Pb to the sediments. This model is used when the sedimentation rate is constant, although it may be appropriate in sites with non-uniform accumulation if results compare with other dating methods (Appleby 2001).
210Pb activities were low in the upper 3 cm of the core, increased by 4 cm, and subsequently declined exponentially to the bottom of the core, although with some variability (discussed below). Application of the CRS model accurately estimated the age of the 137Cs peak within 2 years (1961). Excluding turbidite layers, the sedimentation rate, which was estimated from the mean depth of the 1963 137Cs peak, was 0.29 cm year−1, while the sedimentation rate from the 210Pb age model was 0.73 cm year−1 (1837–2003). If the values from 1 to 3 cm were excluded for the latter calculation, the sedimentation rate was 0.30 cm year−1 (1837–1971). From the 210Pb model, 57 cm corresponded to 1837; the basal age (at 69 cm) could not be accurately estimated without an independent chronostratigraphic marker.
Dates for rapidly deposited layers (RDLs)
Within Crystal Lake, comparison between dates for rapidly deposited layers (RDLs, i.e., turbidites) estimated from the 210Pb age model ± 1 standard deviation (sd), and historical events within the lake’s drainage basin, including fire history in the last century (USDAFS 2008), store construction (Conrad 2003), and the 1878 unnamed fire (Minnich 1987, Goforth and Minnich, 2007)
Estimated date ± 1 sd
Events within the drainage basin
2000 ± 2
2002 Curve Fire
1954 ± 2
1957 Gale Fire
1938 ± 2
1930s store construction
1919 ± 3
1919 San Gabriel River Fire
1866 ± 11
1878 unnamed fire
Dates for RDLs—1, 2, 4 corresponded closely to known dates for fires (Table 3), which burned >25 km2 within the immediate vicinity of the lake’s drainage basin (RDL-1: 2002 Curve Fire, RDL-2: 1957 Gale Fire, RDL-4: 1919 San Gabriel River Fire, fire history from USDAFS 2008). Within RDL-5 (1866 ± 11 year), high charcoal counts suggested fallout from an unnamed fire in 1878 (see Fig. 4d), which was one of the largest and longest fires in the Angeles National Forest (240 km2, burned all summer), and occurred within 20 km of Crystal Lake (Minnich 1987; USDAFS 2008). It is possible the perimeter of the fire was closer to the lake, as the location and area burned were not accurately recorded at the time of the fire; more precise record keeping did not begin until the instigation of fire suppression management in 1895 (Goforth and Minnich 2007). RDL-3 (1938) was the only sediment layer not associated with a fire; however, a spike in total carbonate (32–34 cm, LOI, 950°C >18%, Fig. 4c) suggested the RDL occurred following the 1930s construction of a lakeside store (Conrad 2003), during which cement (i.e., calcium carbonate, Ca(CO3)) was likely deposited into the lake.
The correspondence between the sedimentological record and known historical events suggested the age model for Crystal Lake may be appropriate.
Diagenetic remobilization of Hg in core BBL-1 was investigated by comparing Fe, Al, and Hg levels. Additional metals (e.g., Fe, Al) were not measured for the Crystal Lake cores (CL-1, 2, 4). Previous work indicated Hg chronologies may be confounded by biological reworking of sediments and sorption of Hg onto redox sensitive metals, such as Fe (Rasmussen 1994). However, Lockhart et al. (2000) analyzed Hg in sediment cores from polluted sites and verified sediment total mercury profiles were stable over time, while Rydberg et al. (2008) reported diagenesis did not significantly obfuscate Hg trends in sediment cores over a 30-year period. In core BBL-1, there was a lack of correlation between Fe and Hg levels (r2 = 0.00, p > 0.95, n = 8), while there was a strong correlation between Al and Fe levels (r2 = 0.88, p < 0.01, n = 17), suggesting a low probability that diagenetic remobilization impacted Hg levels.
Hg chronologies and accumulation rates
Big Bear Lake
One explanation for the Hg pulse near the base of the core concerned changes in particle size distribution. Increased concentrations of heavy metals are associated with the smaller size fraction (i.e., silt or clay) due to greater sorption capacity (Bengtsson and Picado 2008; Fukue et al. 2006; Schuster 1991). In BBL-1, minimum Hg concentrations occurred at 52 cm (the base of core BBL-1), where sand, silt, and clay comprised 82, 17, and <1%, respectively. At 45 cm, Hg concentrations were 98 ng g−1 (i.e., a 7.5-fold increase) and the distribution of sand, silt, and clay was 7.6, 81, and 12%, respectively. Hg concentrations were positively correlated with the silt and clay fractions, while negatively correlated with sand (r2 = 0.52, p < 0.01). Changes in particle size reflected a rapid increase in lake level beginning in the 1960s; as lake levels rose, heavier sediment particles were not easily transported to the deeper area of the lake. Based on the age model, the sedimentation rate between 1950 and mid-1960s (32–52 cm) was 1.4 times greater compared to the mid-1960s to the present (0–31 cm) (1.5 cm year−1 vs. 1.1 cm year−1), indicating rapid accumulation of finer grain particles as lake levels increased, which led to increased Hg concentrations.
Two large fires occurred <10 km from Big Bear Lake, (1970 Bear Fire, 1999 Willow Fire) (Table 1a; USDAFS 2008). There was a spike in Hg levels near the top of the core (Fig. 3e–f, 2003 for BBL-1, 2002 for BBL-2), which may be associated with the 1999 fire. There was no Hg spike associated with the 1970 fire, although this was a large fire (209 km2) and occurred closest to the western edge of Big Bear.
Hg levels for Crystal Lake sediments ranged from 57 to 510 ng g−1 (CL-1) and from 50 to 360 ng g−1 (CL-2) (Fig. 5f–g). Within CL-1, Hg levels did not increase monotonically; minimum Hg concentrations (<100 ng g−1) occurred at the base of the core (pre-1867) and near the top of the core (2002). Several spikes in Hg concentrations (400–500 ng g−1) were observed at the following dates: 1916, 1920, 1923, 1936, and 1977, and somewhat higher Hg levels occurred in 1956 (330 ng g−1) and 2003 (290 ng g−1). Hg accumulation rates were calculated for non-RDL layers, since RDLs were deposited instantaneously; only those fluxes during periods of “normal” accumulation were significant (Peter Appleby, personal communication). Hg accumulation rates ranged from 110 to 6,000 μg m−2 year−1; highest rates occurred in ~2002, when sedimentation rates sharply increased (Fig. 6). Compared to Big Bear Lake, average Hg levels in Crystal Lake sediments were nearly 2.5 times higher than Big Bear Lake sediments (CL-1: 220 ± 93 ng g−1, CL-2: 200 ± 85 ng g−1, BBL-1: 92 ± 26 ng g−1, and BBL-2: 78 ± 8.2 ng g−1), and average Hg accumulation rates at Crystal Lake were 3.3 times higher than Big Bear Lake accumulation rates (CL-1: 790 ± 1200 μg m−2 year−1, BBL-1: 240 ± 54 μg m−2 year−1). Within CL-1, Hg and organic content were positively correlated (r2 = 0.27, p < 0.01), but were not correlated within CL-2 sediments (r2 = 0.07, p > 0.20).
Comparison between pre-industrial and modern Hg levels (ng g−1) in California (CA) water bodies
Pre-industrial Hg (ng g−1)
Modern Hg (ng g−1)
Ratio between average pre-industrial and modern Hg levels
Crystal Lake, CAa
Four California lakesb
2, 4, 5, 10
Lake Tahoe, CAc
San Francisco, CAe
60 ± 10
<5 to 20
Modern and pre-industrial Hg accumulation rates were also compared; however far fewer data were available since flux was not calculated for RDLs, which comprised 36 cm of the 69 cm core, and there was no age control for the lower 12 cm of the core. Hg accumulation rates averaged 280 μg m−2 year−1 prior to 1865, while modern accumulation rates (post 1965) averaged 1,900 μg m−2 year−1 (16 times higher). The latter result was strongly influenced by higher sedimentation flux near the top of the core (1–3 cm, Fig. 7b).
Atmospheric deposition of Hgp
Hg levels in soils typically decrease following a fire (Amirbahman et al. 2004; Biswas et al. 2007; DiCosty et al. 2006; Engle et al. 2006; Friedli et al. 2001; Harden et al. 2004; Mailman and Bodaly 2005), while atmospheric Hg levels (i.e., Hgo) increase (Friedli et al. 2003a, b, Sigler et al. 2003). Ash may contain lower Hg levels compared to unburned soil (Biswas et al. 2007), however, Kelly et al. (2006) reported a higher release of total Hg and methylmercury (MeHg) in burned compared to unburned catchments within one year following a fire near Moab Lake (Canada). Veiga et al. (1994) also suggested elevated Hg concentrations in the Brazilian Amazon may be due to increased erosion of Hg-laden soil and ash resulting from slash and burn agricultural methods.
Although RDLs 1, 2, 4, and 5 corresponded to known fire history in Crystal Lake, peak Hg concentrations were not consistently observed within RDLs, and there was no statistical difference between Hg levels within RDLs (n = 6) and non-RDL sediments (n = 1) (ANOVA, p > 0.05). This implied that Hg was just as likely to be deposited during high erosional activity, as during “normal” periods of sedimentation. Like BBL-1, Hg was positively associated with the silt and clay fractions and inversely correlated with sand (CL-1: r2 = 0.51, p < 0.01, for BBL-1: r2 = 0.52, p < 0.01); however, there was no statistical difference between RDL and non-RDL layers with respect to particle size (p > 0.40).
Higher Hg concentrations in Crystal Lake sediments, and lower Hg enrichment compared to other sites in California (Table 4) suggested atmospheric deposition of Hgp following wild fires may be important. Wildfires and biomass burning are major sources of air pollution, including particulate matter (PM) (Sapkota et al. 2005; Zhang et al. 2008). Friedli et al. (2003a, b) reported most Hg (>88%) emitted during a wildfire is in the form Hgo, while the remaining Hg is bound to particulates. However, Hgp includes many Hg species, including Hgo. Feng et al. (2004) analyzed inorganic mercury species associated with airborne particulate matter, and reported the following range of Hg species between triplicate tests: Hgo (19–38%), HgCl2 (19–26%), HgO (28–49%), and HgS (7.8–11%). Although Hgp is typically a small fraction of total Hg in a smoke plume, in the presence of high levels of particulates the ratio of Hgp:Hg may increase. Given the estimated levels of particulates released during a fire (6,000–13,000 tons of PM2.5, from Zhang et al. 2008), not all Hgo likely enters the global circulation cycle; particulates may scavenge Hgo, which may then be deposited directly to the earth’s surface, decreasing the tropospheric residence time of emitted Hg. In addition, there may be a time delay for erosion following fires, especially in California, where precipitation levels are low and occur 4–6 months after the fire season, while particulates from a fire may be deposited immediately after a fire. Hg levels spike just before the occurrence of RDLs 1,5, and 6 (Fig. 4), which may reflect atmospheric deposition of Hgp prior to erosion of sediments. Witt et al. (2009) reported total Hg levels in precipitation significantly increased following fires (samples collected 3–47 days postburn). Since Hgp is readily scavenged by rain, these results suggested Hg released from vegetation and soil during a fire was deposited through wet deposition of Hgp. Findings from this study indicated dry deposition of Hgp was also important.
Historical wildfires regularly subsumed the forest surrounding Crystal Lake, unlike the area around Big Bear Lake, which was spared the impact of fires. Despite the close proximity of the two lakes, average Hg sediment concentrations at Crystal Lake were 2.2–2.8 times higher than Big Bear Lake sediments, while average Hg accumulation rates at Crystal Lake were 3.3 times greater. During a fire most Hg is released from vegetation and soil as Hgo, and may affect the global cycling of Hg. Findings from this study suggest high levels of Hg remain in the vicinity following a fire, which may be deposited through dry deposition of Hgp. The impacts of fires on Hg cycling should be further explored, since wild fires occur annually in this region, and may help explain the prevalence of Hg impairments in southern California water bodies. Crystal Lake and Big Bear Lake are located ~40-km apart, and results indicated atmospheric deposition of Hgp following fires was confined near the fire source.
This research was funded by the Big Bear Municipal Water District, the American Chemical Society/Petroleum Research Fund (#41789-GB8) and the NSF (EAR-0318511) (to M. Kirby). This work was also funded by a NSF Career Award (BES-0378483) (to J. Jay), and a NSF International Research Fellowship (#0802014) (to S. Rothenberg). M. DeRose received an Undergraduate Research Award from California State University, Fullerton and a Grants-in-Aid-of-Research from Sigma Xi. This research was also partially supported by the State Key Laboratory of Environmental Geochemistry, Institute of Geochemistry, Chinese Academy of Sciences, in Guiyang, China. The authors thank the personnel at the Angeles National Forest Service, Eric Zhang (from the San Francisco Estuary Institute) and Sharon Landau. The authors sincerely appreciate assistance from Prof. Peter Appleby, and also acknowledge the comments from two anonymous reviewers, which greatly improved this manuscript.
This article is distributed under the terms of the Creative Commons Attribution Noncommercial License which permits any noncommercial use, distribution, and reproduction in any medium, provided the original author(s) and source are credited.
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