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a Dep. of Plant Science, Wageningen Univ. and Research Centre, Haarweg 333, 6709 RZ Wageningen, The Netherlands, present address: Brouwer Environmental and Agricultural Consultancy, Wildekamp 32, 6721 JD Bennekom, The Netherlands
b Dep. of Primary Industry, P.O. Box 219, Maryborough, Qld 4650, Australia
brouwbar{at}bos.nl
| ABSTRACT |
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Abbreviations: AWHC, available water holding capacity
| INTRODUCTION |
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During the past 50 yr a number of studies have shown that coarse rock fragments can hold considerable volumes of water; such fragments, or indeed the weathering bedrock itself, should not be ignored when calculating the AWHC of a stony soil (e.g., Coile, 1953; Berger, 1976; Hanson and Blevins, 1979; Arkley, 1981; Flint and Childs, 1984; Montagne et al., 1992; Jones and Graham, 1993; Ugolini et al., 1996; Oyonarte et al., 1998).
While the studies mentioned were concerned with pieces of fresh and weathering rock, under intermittent saturated conditions coarse fragments in the soil can also be formed by Fe cementation of fine earth material. The ferruginous nodules or pisolithic ironstone gravel that can thus be formed are quite commonly found in hydromorphic soils and Paleosols of the tropics and subtropics, in horizons of a range of textures (Tardy, 1992).
To show that the water retention properties of ironstone gravel, too, can appreciably affect the AWHC of soils, we present data from a field study in western Victoria, Australia. Correlations are also shown to exist between AWHC on the one hand and the depth of occurrence and magnetic properties of the ironstone gravel on the other hand. To the best of our knowledge, somewhat similar data have previously only been published in a francophone journal from West Africa (Boa, 1990, 1993; Assa and Boa, 1990), based largely on an unpublished report (Boa, 1983). The francophone journal has a very limited distribution and is not included by abstracting services. In addition, Boa's approach is quite different from ours, and, for instance, does not examine correlations between AWHC and magnetic properties and depth of occurrence of the ironstone gravel. We only happened to hear about Boa's publications when the senior author moved to West Africa, well after our own measurements had been made.
There are a number of definitions of AWHC as determined in the laboratory. In this note we define the AWHC of the soil as the water being held by an undisturbed soil core at tensions between -20 and -1500 kPa, in cubic meters per cubic meter of soil core. Similarly, the AWHC of the sieved out coarse fragments in the soil is the water being held by those fragments at tensions between -20 and -1500 kPa, in cubic meters per cubic meter of coarse fragment.
| Materials and Methods |
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| Methods |
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The soil water retention curves of the undisturbed cores were determined on a suction table for potentials down to -20 kPa. Although in the determination of AWHC the upper limit can vary between -10 and -33 kPa, the limit of -20 kPa was the standard used in the laboratories of the Land Protection Division in Victoria; it is the limit used here in the calculation of AWHC values.
Water contents at -1500 kPa were determined in a pressure chamber as described by Klute (1986)(p. 648), using the <2-mm fraction fine earth. The fine earth fraction was isolated by grinding the air-dry peds from the undisturbed cores with a mortar and pestle and then using a 2-mm sieve to separate the fine earth from the ironstone gravel. For a pressure potential of -1500 kPa, this can be an acceptable method for determining soil water content (Elrick and Tanner, 1955, as cited in Klute, 1986).
Water contents at -20 kPa were calculated on the basis of the oven-dry weight of the whole core minus the oven-dry weight (not the moist weight) of the ironstone gravel. In this standard calculation (see Klute, 1986), it is implicitly assumed that the ironstone gravel holds no water at -1500 kPa. This means that any water the ironstone gravel does hold at -1500 kPa is wrongly assumed to have been held by the fine earth at between -20 and -1500 kPa. In our case, in samples with large amounts of ironstone gravel (up to 27% by volume), this method of calculation resulted in inexplicably high AWHC values for the fine earth fraction. We therefore decided to separately measure the water content at -1500 kPa of some of the ironstone gravel that had not yet been oven dried. For each of the layers near the surface, ironstone gravel from three different cores was used for this purpose. At 0.58 m depth, ironstone gravel from only one core was available, and at 0.83-m depth ironstone gravel from only two cores was available.
The ironstone gravel was scrubbed to remove adhering soil, soaked in water at room temperature for 3 d, put in the pressure chamber at -1500 kPa until equilibrium water content had been reached, weighed, oven dried, and weighed again. Dry bulk densities were subsequently determined by rapid immersion of the oven-dried ironstone gravel samples of known weight into water in a graduated cylinder. The accuracy of these simple bulk density determinations can be affected by water entering the pores of the ironstone gravel. The bulk density determinations were therefore checked against the pore volume of the ironstone gravel, known from saturated water content determinations, and the specific densities of the constituent minerals of the ironstone gravel: if the bulk density determination is precise, it will equal (specific density) x (1 - fractional pore volume).
Because the water contents of the ironstone gravel at -1500 kPa were all found to be very high, it was decided to carry out further water retention determinations on the same ironstone gravel samples, this time separated into magnetic and nonmagnetic fractions. Water contents at -20 kPa were determined by embedding known weights of ironstone gravel in known amounts of diatomaceous earth of high uniformity and with known water retention characteristics. The uniformly fine pore system of the packed diatomaceous earth ensures good water supply to, and even withdrawal of water from, the whole surface of the ironstone gravel. The samples with the ironstone gravel and the diatomaceous earth were first saturated for several days (initially by capillary action to minimize air entrapment) and then put on the suction table at -20 kPa until equilibrium was reached. The samples were then weighed. Water contents (kg kg-1) of the ironstone gravel samples were calculated using the known water content of the diatomaceous earth at -20 kPa. Water contents at -1500 kPa and apparent bulk density of the magnetic and nonmagnetic ironstone gravel fractions were then determined using a pressure chamber, oven, and graduated cylinder as described above.
| Results |
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The results of the second set of water retention determinations are presented in Table 3 . The magnetic and nonmagnetic ironstone gravels showed clear differences in apparent bulk density (P < 0.01) and in distribution with depth: magnetic ironstone gravel was found almost exclusively in the A and E horizons, where it constituted up to one-half of the total ironstone gravel fraction. The high apparent bulk density of the magnetic ironstone gravel is the reason for the high average bulk density of 3.1 Mg m-3 for the combined ironstone gravel in the A and E horizons (0.00.30 m), compared with only 2.5 to 2.6 Mg m-3 in the B horizon (0.3 to >0.9 m): see Table 2. The AWHC values of both magnetic and nonmagnetic ironstone gravel varied between 0.03 and 0.15 m3 m-3.
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| Discussion |
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The accuracy of the results of the water retention calculations on a volume basis depend of course on the accuracy of the apparent bulk density determinations for the ironstone gravel. The apparent bulk densities can be checked against total pore volume and the specific densities of the minerals present in the ironstone gravel. In the ironstone gravel, with almost no large pores, total accessible pore volume will be somewhat, but not much, greater than volumetric water content at -20 kPa. On the basis of visual inspection of scanning electron microscope images of a number of pieces of ironstone gravel from the same site, we have estimated a conversion factor of 1.1. The volumetric water contents at -20 kPa of 0.16 to 0.36 m3 m-3 (Table 3) thus convert to total pore volumes of 0.17 to 0.40. The average apparent dry bulk densities of the nonmagnetic ironstone gravel of 2.3 to 2.9 Mg m-3 then convert to specific densities of 3.3 to 4.2 Mg m-3. This is very similar to the specific density of 3.6 to 4.0 Mg m-3 of goethite, the dominant cementing Fe mineral in the nonmagnetic ironstone gravel from Gatum (R.W. Fitzpatrick, 1995, unpublished data). In the same way, the apparent bulk density of the magnetic ironstone gravel of 3.4 Mg m-3 and the volumetric water contents at -20 kPa of 0.13 to 0.15 m3 m-3 (Table 3) convert to specific densities of 4.2 to 4.8 Mg m-3. This is close to the specific density of 4.9 to 5.3 Mg m-3 of maghemite and hematite, the dominant Fe minerals in the magnetic ironstone gravel, which also contains some lighter goethite (R.W. Fitzpatrick, 1995, unpublished data). Assa and Boa (1990) also reported apparent bulk densities of up to 2.9 for ironstone gravel from Ivory Coast, without distinguishing between magnetic and nonmagnetic ironstone gravel.
The increase with depth in water content of the ironstone gravel at both -20 and -1500 kPa suggests an increase in porosity with depth. Similar increases in ironstone gravel porosity with depth can be inferred from the data of Tiessen et al. (1991): ironstone gravel taken by them from >0.65-m depth at a site in Ghana had an effective cation exchange capacity that was twice as high as that of ironstone gravel taken from the 0.3- to 0.4-m depth: 32 vs. 16 mmol kg-1. Mineralogy being the same (kaolinite dominated), a greater effective cation exchange capacity indicates a greater reactive surface and thus arguably a greater porosity of the ironstone gravel from greater depth.
The data in Table 2 show that, when calculating AWHC for the gravelly soils, ignoring the water held in the ironstone gravel at -1500 kPa led to overestimation of the AWHC by 0.012 to 0.066 m3 m-3. Put differently, the real AWHC of the bulk soil (including ironstone gravel) in individual soil layers, was only 60 to 93% of the AWHC calculated while ignoring the water held by the ironstone gravel at -1500 kPa. As mentioned above, the latter calculations are based on the incorrect, but commonly held, assumption that the water still held by the ironstone gravel at -1500 kPa or less had been held by the fine earth fraction at between -20 and -1500 kPa. Using the data in the 13th column of Table 2, the real AWHC of the top 1.0 m of an average profile at our field site in Gatum is estimated to be
129 mm. Ignoring the water held by the ironstone gravel at less than -1500 kPa would have led one to assume that it was 162 mm (15th column of Table 2).
The data in Table 3 show that the AWHC values of both the magnetic and nonmagnetic ironstone gravels varied between
0.03 and 0.15 m3 m-3. Boa (1983), studying ironstone gravels from Ivory Coast, also measured AWHC values of up to 0.15 m3 m-3 (and volumetric water contents at saturation of up to 0.34 m3 m-3). This is similar to the AWHC values reported for rock fragments by Hanson and Blevins (1979), Flint and Childs (1984), Montagne (1992), and Jones and Graham (1993). Given the formation process of ironstone gravel (very slow precipitation, initially as bridges between particles in the soil, often followed by the formation of a weathered rind on the outside), significant porosity of ironstone gravel is not unexpected. However, one would expect the porosity of the ironstone gravel to be less than the porosity of the fine earth it is formed in. Comparison of the AWHC values for whole cores in Table 2 with those for the ironstone gravel only in Table 3 and comparison of the water contents of gravel and fine earth at -1500 kPa indicate that the ironstone gravel is indeed less porous than the fine earth.
The results of the two determinations of volumetric water content of ironstone gravel at -1500 kPa (Tables 2 and 3) show good agreement. That the water contents measured the second time are slightly lower than those measured the first time, particularly for samples from surface horizons, may be due to partial rubbing off of the weathered rind of the ironstone gravel during repeated handling. The second time the ironstone gravel had also already been oven dried once. The changes in bulk density and water content of the ironstone gravel with depth indicate that not all ironstone gravel is the same: differences in genesis, mineralogy, and weathering can cause differences in bulk density and water retention. This is also demonstrated by the differences in bulk density and water retention between the magnetic and nonmagnetic ironstone gravel fractions. Similar observations about the effects of genesis on ironstone gravel water holding characteristics were also made by Boa (1990) about ironstone gravels from Ivory Coast.
| Conclusions |
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In traditional determinations of soil water retention curves, where ironstone gravel is assumed not to hold any water at all, the water actually held by the ironstone gravel at less than -1500 kPa is wrongly assumed to be held by the fine earth fraction at -20 to -1500 kPa. If there are significant amounts of ironstone gravel present in the soil, these wrong assumptions can lead to considerable overestimation of the AWHC of the bulk soil. In our own most extreme example, a horizon with 27% ironstone gravel by volume, the actual AWHC was 0.097 m3 m-3. Ignoring the water held by the ironstone gravel at less than -1500 kPa would have led to the conclusion that the AWHC was 0.163 m3 m-3, an overestimation by 67% (factor 1.67). Similarly, the real AWHC of the top 1.0 m of an average profile was calculated to be 129 mm. Ignoring the water held by the ironstone gravel at less than -1500 kPa would have led one to estimate that it was 162 mm. This difference of 33 mm in water storage capacity can greatly affect perceived options for improving land management at our field site in the Dundas Tableland area (average rainfall 630 mm yr-1): severe dryland salinity problems at the site are thought to be caused by an increase in annual groundwater recharge of only 20 to 25 mm.
The above facts demonstrate that when soils containing ironstone gravel are present, the water retention characteristics of such ironstone gravel should not be ignored in field studies or simulation modeling of the water balance. In land evaluation studies, one should also not automatically assume that high ironstone gravel contents will have a negative effect on crop growth because of reduced water availability.
It seems unlikely that changing the upper tension limit for the AWHC determination from -20 to -10 or -33 kPa would have led to substantially different conclusions.
| ACKNOWLEDGMENTS |
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| NOTES |
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Received for publication July 23, 1999.
| REFERENCES |
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