Abstract
- Top of page
- Abstract
- 1. Introduction
- 2. Field Site
- 3. Methods
- 4. Results
- 5. Discussion
- 6. Conclusions
- Appendix A:
- Acknowledgments
- References
- Supporting Information
[1] This work examined the plot-scale differences in soil-water retention caused by wildfire in the area of the 2010 Fourmile Canyon Fire in the Colorado Front Range, United States. We measured soil-water retention curves on intact cores and repacked samples, soil particle-size distributions, and organic matter content. Estimates were also made of plant-available water based on the soil-water retention curves. Parameters for use in soil-hydraulic property models were estimated; these parameters can be used in unsaturated flow modeling for comparing burned and unburned watersheds. The primary driver for measured differences in soil-water retention in burned and unburned soils was organic matter content and not soil-particle size distribution. The tendency for unburned south-facing soils to have greater organic matter content than unburned north-facing soils in this field area may explain why unburned south-facing soils had greater soil-water retention than unburned north-facing soils. Our results suggest that high-severity wildfire can “homogenize” soil-water retention across the landscape by erasing soil-water retention differences resulting from organic matter content, which for this site may be affected by slope aspect. This homogenization could have important implications for ecohydrology and plant succession/recovery in burned areas, which could be a factor in dictating the window of vulnerability of the landscape to flash floods and erosion that are a common consequence of wildfire.
1. Introduction
- Top of page
- Abstract
- 1. Introduction
- 2. Field Site
- 3. Methods
- 4. Results
- 5. Discussion
- 6. Conclusions
- Appendix A:
- Acknowledgments
- References
- Supporting Information
[2] The water retention of soils is commonly represented using the constitutive relationship between volumetric soil-water content and matric potential (i.e., the soil-water retention curve). This water retention relationship is critical for the dynamics of soil moisture, soil-plant-water relations, net infiltration/groundwater recharge, and water exchange between the soil and atmosphere [e.g.,Nimmo, 2009]. Soil-water retention curves depend on many factors such as soil texture (i.e., the particle-size distribution) [Salter et al., 1966; Gupta and Larson, 1979; Arya et al., 1999; Nimmo et al., 2007], organic matter content [Gupta and Larson, 1979; Vereecken et al., 1989], soil structure [Jamison, 1953; Nimmo, 1997], and ambient soil temperature [Nimmo and Miller, 1986].
[3] Wildfire can profoundly impact soil properties by alteration or consumption of organic matter and reduction of structure and porosity [Certini, 2005; Mataix-Solera et al., 2011], which in turn impacts the soil-water retention curve. The first-order controls on fire effects on soil properties are the fire intensity (i.e., rate of thermal energy production) and duration; these variables are determined by factors such as fuels, atmospheric conditions, and topography [Certini, 2005]. The combination of intensity and duration (i.e., fire severity), along with second-order controls like soil-water content at the time of wildfire, determines the warming of the soil at depth. The heat impulse from fire rarely reaches 20–30 cm below land surface and temperatures greater than 150°C are seldom achieved deeper than 5 cm [DeBano, 2000]. Organic matter consumption, which is known to affect water retention in fire-impacted soils [e.g.,Stoof et al., 2010], commences between 200°C and 250°C and full combustion can occur by 460°C [Giovanni et al., 1988], with intermediate temperatures like 220°C still producing almost 40% loss of organic matter [Fernàndez et al., 1997]. At temperatures between 250°C and 500°C, black carbon is produced [Baldock and Smernik, 2002]. The organic geochemistry of the conversion and destruction of organic matter in the presence of soil heating is highly complex [González-Pérez et al., 2004; Miltner and Zech, 1997] and beyond the scope of this work.
[4] Soil structural stability can decrease because of the destruction of organic cements [Badìa and Martì, 2003], which changes the particle-size distribution [Giovannini and Lucchesi, 1997]. Aggregation of fines (i.e., clay and silt size fractions) from wildfire can lead to a “coarsening” of the particle-size distribution, resulting in a distribution with a higher sand fraction [Ulery and Graham, 1993; Molina and Sanroque, 1996; Giovannini and Lucchesi, 1997]. The study by Stoof et al. [2010]found a fining of the particle-size distribution, with a shift to more clay and silt sizes. Some studies have not observed particle-size distribution shifts after wildfire [Oswald et al., 1999].The prewildfire particle-size distribution may be the primary control on the directionality and magnitude of wildfire effects on particle-size distributions. Pore-size distribution changes can be restricted to the very near surface soils, for example,Mallik et al. [1984]found that particle-size distribution changes were restricted to the upper 2 cm of soil. Shifts in particle-size distribution could be responsible for soil-water retention differences following wildfire.Boix-Fayos [1997]attributed reduced postwildfire soil-water retention to decreased clay contents (i.e., coarsening of the particle-size distribution). Increases in bulk density reported after wildfire [Giovannini et al., 1988; Andreu et al., 2001; Stoof et al., 2010] also imply a loss of soil porosity, which should decrease the volumetric water content at saturation.
[5] The incorporation of ash into soil is an additional factor potentially impacting soil-water retention following wildfire. FollowingScott [2010] and Bodí et al. [2011], ash is defined as solid residual material from biomass combustion consisting of charred organic matter, charcoal, and mineral particles. As noted by Woods and Balfour [2010], the impact of ash incorporation into soil on soil-hydraulic properties (such as soil-water retention) hinges on the soil particle-size distribution relative to the ash particle-size distribution, which determines whether the ash has a “clogging” effect.
[6] Wildfire-affected soil can have enhanced soil-water repellency, which in turn affects water retention. Effects of soil-water repellency on soil-water retention are not binary in that soil-water retention curves affected by soil-water repellency can lie in a “transition zone” between the end members of being completely hydrophilic versus hydrophobic [Dekker et al., 2001]. Phenomena such as hysteresis can also be enhanced by soil-water repellency [Kobayashi et al., 1996; Miyata et al., 2007]. As a further complication, soil-water repellency is soil-water content dependent [Goebel et al., 2004; Regalado and Ritter, 2005; de Jonge et al., 2007], suggesting that a soil-water repellency characteristic curve may be needed to fully characterize the hydraulic properties of water-repellent soils [Bachmann et al., 2007; Karunarathna et al., 2010a, 2010b]. An alternative is to measure soil-water retention using traditional methods and then effects of repellency (if present in a given soil) may be incorporated in an “effective” sense [e.g.,Miyata et al., 2007].
[7] Previous research on fire impacts on water retention has relied on both laboratory experiments [e.g., Badìa and Martì, 2003; García-Corona et al., 2004; Stoof et al., 2010] and field-sampling studies [e.g.,Boix-Fayos, 1997; Alauzis et al., 2004; Kitzberger et al., 2005; Silva et al., 2006]. Results from some of these selected studies are summarized in Table 1. Comparison of the different studies in Table 1shows that nearly all investigations have found reductions in soil-water retention following wildfire based on soil-water contents (θ) at saturation, field capacity, and permanent wilting point.
Table 1. Summary of the Findings of Selected Studies Examining Wildfire Impacts on Soil-Water Retentiona| Study | Soil-Water Retention Impact | θPermanent wilting point | Full Range of ψ | Number of Samples | Sample Type | Fire Type | Δ Unburned − Burned PAWb,c (%) |
|---|
| θSaturation | Field Capacity |
|---|
|
| Mallik et al. [1984] | G | G | G | | 6 | Int. | Exp. | −42.6 |
| Boix-Fayos [1997] | L | L | L | | 60 | Dist. | Wild | |
| Badìa and Martì [2003] | L | L | | | 8 | Dist. | Lab. | |
| Alauzis et al. [2004] | | L | | | 6 | Dist. | Wild | |
| Kitzenberger et al. [2005] | L | L | L | | 4 | Dist. | Wild | 11.1 |
| González-Pelayo et al. [2006] | | | | | 9 | Dist. | Exp. | |
| Under vegetation canopy | | L,d Ge | Ld,e | | | | | −34.4,d −118.0e |
| Bare soil | | L,d Ge | L,dGe | | | | | 7.4,d 0e |
| Silva et al. [2006] | L | L | L | | 4 | Int. | Exp. | 0 |
| Are et al. [2009] | = | = | = | | 20 | Int. | Exp. | 8.0,f 4.8g |
| Stoof et al. [2010] | | | | L | 25 | Dist. | Lab. | −9.3 |
| This study | G,d,h L,e,h Li | G,h Li | G,h Li | G,d,h L,e,h Li | 7 | Int. | Wild | −15.7,h −49.4,h 32.9,i 28.8i |
[8] The finely controlled conditions of soil heating in laboratory experiments used to simulate wildfire impacts are useful for precise examination of temperature effects on soil-water retention and such controlled experiments are difficult to replicate in field studies [Stoof et al., 2010]. Controlled experiments, however, typically use sieved and repacked samples where soil structure has been substantially altered. Recent work has also suggested that furnace heating may not adequately represent wildfire conditions [Bodí et al., 2011]. Therefore, the importance of field studies to complement laboratory experiments motivated us to collect and analyze field samples of soils both affected and unaffected by wildfire. Because the field area selected in this work has mountainous topography, wildfire may differentially impact soils across the landscape because of differences in soil development, vegetation communities, soil organic matter content, and soil-water retention.
[9] The principal objective of this work was to examine soil-water retention differences between burned and unburned soils along with factors that impact water retention such as particle-size distribution and organic matter content. Here we use “burned” to describe soils that have been fire affected and “unburned” for soils in a prefire state. Water-retention differences are organized with respect to the two disparate aspects that dominate the field site, which are north- (NF) and south-facing (SF). An additional objective of this work was to provide unsaturated hydraulic property model parameters for use in unsaturated flow modeling [e.g.,Šimůnek et al., 2008] and models of coupled surface water/groundwater flow [e.g., VanderKwaak, 1999; Kollet and Maxwell, 2006; Qu and Duffy, 2007; Sudicky et al., 2008; Furman, 2008] for application to wildfire-impacted areas. The paucity of unsaturated hydraulic property model parameters for burned watersheds makes this study unique. This work was conducted using single cores taken from six research plots (Figure 1). On the NF slope, there was one unburned plot (UBNF), two burned plots at different hillslope positions at the ridge (NFR) and midslope (NFM), and an ash sample from the NFM plot. On the SF slope, there was one unburned plot (UBSF) and two burned plots at ridge (SFR) and midslope (SFM) positions.
2. Field Site
- Top of page
- Abstract
- 1. Introduction
- 2. Field Site
- 3. Methods
- 4. Results
- 5. Discussion
- 6. Conclusions
- Appendix A:
- Acknowledgments
- References
- Supporting Information
[10] The field site for this effort was the 2010 Fourmile Canyon Fire near Boulder, Colorado, United States [Ebel et al., 2012; Moody and Ebel, 2012]. The fire began on 6 September 2010 and was contained on 13 September 2010 [Fourmile Emergency Stabilization Team (FEST), 2010]. High winds, rugged topography, and spatially variable vegetation contributed to a patchy network of low, moderate, and high soil burn severities (after Keeley [2009]) spread over approximately 2500 ha [FEST, 2010]. Soil burn severity focuses on wildfire-caused changes in physical, hydrologic, and biologic properties and includes, for example, color, structure, and infiltration capacity [Parsons et al., 2010].This investigation of the differences in soil-water retention caused by wildfire and aspect was facilitated by selection of burned and unburned sites with NF and SF aspect slopes at the southern edge of the fire (Figure 1). Despite being located at the edge of the fire perimeter, the burned sites were of relatively high severity [FEST, 2010] owing to a reversal of wind direction coupled with high wind velocities. The soils at the area are part of the Allens Park member of the Fern Cliff-Allens Park-Rock outcrop complex and are nonsaline and nonsodic [Moreland and Moreland, 1975]. The soils are classified as frigid Lamellic and Typic Haplustalfs [United States Department of Agriculture (USDA), 2010]. Aspect affects soil horizon development in the field area because SF aspects tend to be warmer and drier while NF aspects tend to be cooler and wetter [Veblen and Lorenz, 1991], resulting in NF soils having relatively thin O and E horizons underlain by B and C horizons (Cryalfs or Ustalfs) and SF soils having thicker A and E horizons underlain by B and C horizons (Cryolls or Ustolls) [Birkeland et al., 2003]. The parent material for the colluvial/residual soils was the Boulder Creek granodiorite, with very limited exposures of a diabase from a feature known as the Iron Dike [Gable, 1980]. The prewildfire vegetation was typical of Montane ecosystems in the Rocky Mountain Foothills and aspect dependent, with NF slopes consisting of aspen (Populus tremuloides), Rocky Mountain douglas fir (Pseudotsuga menziesii subspecies glauca), and limber pine (Pinus flexilis) and with SF slopes having more sparse forests of ponderosa pine (Pinus pondersosa) and Rocky Mountain juniper (Juniperus scopulorum). The most recent major fire in the Fourmile Canyon area was in 1860 [Graham et al., 2012], which is longer than the mean wildfire return interval in low elevation Northern Colorado forests [Veblen et al., 2000; Sherriff and Veblen, 2007]. The mature stands of vegetation (i.e., trees) and robust understory that developed during this long period between major fires may have contributed to fire severity.
3. Methods
- Top of page
- Abstract
- 1. Introduction
- 2. Field Site
- 3. Methods
- 4. Results
- 5. Discussion
- 6. Conclusions
- Appendix A:
- Acknowledgments
- References
- Supporting Information
[11] To cover the full range of soil-water contents (θ) from saturation to near-oven dryness, a variety of measurement techniques were used for the burned and unburned soils and the ash. The majority of retention measurements were conducted in the laboratory using intact cores with a combination of a hanging column [Dane and Hopmans, 2002a], pressure plate [Dane and Hopmans, 2002b], dewpoint potentiometer [Gee et al., 1992], and a relative-humidity-controlled chamber [Nimmo and Winfield, 2002]. Portions of each sample were removed from the core for the dewpoint potentiometer and relative-humidity-controlled chamber measurements. The matric potential (ψ) ranges for each laboratory technique and sample equilibration times are given in Table A1. Samples (N= 1 per experimental plot) were collected just below the surface (i.e., between one and two and 7–8 cm depth) by digging a small trench and then driving in the coring device parallel to the ground surface in the upslope direction and then excavating the intact core. The presence of many stones in the subsurface required multiple coring attempts to retrieve an intact sample without abundant rocks. At the UBNF plot, cores were taken below the several-centimeter thick litter duff layer into soil that was primarily in the B horizon. The UBSF plot cores were from the A horizon. The north-facing burned cores from the NFM and NFR plots appeared to be mixed E and B horizons and the south-facing burned cores appeared to be primarily from the A horizon. Cores from the field plots were 6 cm in diameter and 20 cm long. These larger cores were subsampled for the laboratory measurements to average dimensions of 4 cm diameter and 7–10 cm length. The ash-retention curve measurements were conducted on disturbed samples that were repacked to a field-measured bulk density, rather than on intact cores because the ash layer present immediately after the fire when ash samples were collected was only 1.8 cm thick, on average [Ebel et al., 2012]. Core samples were saturated for 24 h under vacuum and then left saturated for an additional 2 days. Miyata et al. [2007] noted that saturation of samples longer than 24 h tended to overcome water repellency.
[12] Additional retention measurements were conducted on disturbed soil samples to better characterize dry-end retention (i.e., soil-water content below 0.05 m3 m−3). These additional measurements on disturbed samples, used separately for calibration of Decagon 5TE soil-water content sensors (Decagon Devices), were taken at depths 5–10 cm deeper than the intact cores, which may have slight impacts on physical and hydrologic properties of those samples. These repacked samples were wetted in a controlled fashion, rather than dried like the intact cores, although the repacked samples were taken in the dry end of the soil-water retention curve with the largest matric potential near −1 × 104 cm where hysteresis effects are less pronounced. Retention curve analysis of the intact cores was conducted by D. B. Stephens and Associates in Albuquerque, New Mexico. The dewpoint potentiometer analysis of the repacked samples was conducted at the U.S. Geological Survey Soil Laboratory in Boulder, Colorado. The computer program RETC [van Genuchten et al., 1991] was employed to estimate van Genuchten [1980] parameters. Parameters for the Rossi and Nimmo [1994]junction model approach for representing soil-water retention were fit using nonlinear least-squares optimization in the MATLAB software package. Field capacity remains problematic to define because benchmark pressure approaches do not apply across the full range of soils [Meyer and Gee, 1999], and field capacity can be a dynamic rather than a static hydraulic property [Ahuja et al., 2008]. Field capacity was taken to be the soil-water content at a matric potential of −340 cm, which is 0.33 bars, a commonly used value [Twarakavi et al., 2009] and the permanent wilting point was taken to be the soil-water content at a matric potential of −1.6 × 104 cm [Koorevaar et al., 1983]. While field capacity can differ between soils [e.g., Romano and Santini, 2002] and the permanent wilting point can differ between plant species, using −340 cm and −1.6 × 104 cm, respectively, was consistent with other studies in Table 1, and thus facilitated comparison between our work and results from previous researchers across the scientific community.
[13] Loss on ignition (LOI) measurements to determine organic matter content [Dean, 1974; Heiri et al., 2001] were conducted at 550°C for 2 h based on laboratory experiments, to determine the duration to achieve no appreciable change in mass. The LOI technique, while not the most robust method for analyzing the amount of soil organic matter, was useful here for comparing relative differences between samples. Measurement of the particle-size distribution was conducted using standard dry-sieving techniques for standard class sizes [Guy, 1969] down to 63 μm. Particle size distributions for the fraction less than 63 to 0.04 μm were analyzed using a Coulter LS-230 optical diffraction apparatus [Gee and Or, 2002]. Further information on this particle-size determination technique can be found inWinfield [2003]. Analysis of particle size and LOI was performed on bulk samples taken 0–5 cm below the surface adjacent to core samples to achieve enough sample volume to run replicate samples.