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REPRINT – Nimmo, J.R., 2004, and Pore Size Distribution, in Hillel, D., ed. Encyclopedia of in the Environment: London, Elsevier, v. 3, p. 295-303.

Porosity and Pore Size Distribution the medium. Thus we consider a single, con- J. R. Nimmo, U.S. Geological Survey, tiguous pore space within the body of . In Menlo Park, CA 94025, USA general, the pore space has fluid pathways that Key Words: soil structure, aggregation, , are tortuous, variably constricted, and usually soil hydraulic properties, , soil highly connected. Figure 1 is an example of a retention, hysteresis, tillage, soil , two-dimensional cross section of soil pore solute transport. space.

The pore space is often considered in terms A soil’s porosity and pore size distribution of individual pores--an artificial concept that characterize its pore space, that portion of the enables quantifications of its essential charac- soil’s volume that is not occupied by or iso- ter. Though many alternatives could serve as a lated by material. The basic character of basis for the definition of pores and their sizes, the pore space affects and is affected by criti- in and these are best cal aspects of almost everything that occurs in conceptualized, measured, and applied with the soil: the movement of water, air, and other respect to the fluids that occupy and move fluids; the transport and the reaction of chemi- within the pore space. cals; and the residence of roots and other biota. By convention the definition of pore space ex- cludes fluid pockets that are totally enclosed Porosity within solid material—vesicles or vugs, for example, that have no exchange with the pore Porosity φ is the fraction of the total soil space that has continuity to the boundaries of volume that is taken up by the pore space. Thus it is a single-value quantification of the amount of space available to fluid within a specific body of soil. Being simply a fraction of total volume, φ can range between 0 and 1, typically falling between 0.3 and 0.7 for soils. With the assumption that soil is a continuum, adopted here as in much of soil science litera- ture, porosity can be considered a function of position.

Porosity in natural soils The porosity of a soil depends on several factors, including (1) packing , (2) the breadth of the size distribution (polydisperse vs. monodisperse), (3) the shape of , and (4) cementing. Mathemati- cally considering an idealized soil of packed

Figure 1. Cross section of a typical soil with pore uniform spheres, φ must fall between 0.26 and space in black. This figure would lead to an under- 0.48, depending on the packing. Spheres ran- estimate of porosity because pores smaller than domly thrown together will have φ near the about 0.1 mm do not appear. (Adapted from Lafe- ber, 1965, Aust. J. Soil Res., v. 3, p. 143.) middle of this range, typically 0.30 to 0.35. A with grains nearly uniform in size

1 REPRINT – Nimmo, J.R., 2004, Porosity and Pore Size Distribution, in Hillel, D., ed. Encyclopedia of Soils in the Environment: London, Elsevier, v. 3, p. 295-303.

(monodisperse) packs to about the same poros- Porosity is often conceptually partitioned ity as spheres. In a polydisperse sand, the fit- into two components, most commonly called ting of small grains within the pores between textural and structural porosity. The textural large ones can reduce φ, conceivably below component is the value the porosity would the 0.26 uniform-sphere minimum. Figure 2 have if the arrangement of the particles were illustrates this concept. The particular sort of random, as described above for granular mate- arrangement required to reduce φ to 0.26 or rial without cementing. That is, the textural less is highly improbable, however, so φ also porosity might be about 0.3 in a granular me- typically falls within the 0.30-0.35 for dium. The structural component represents polydisperse . Particles more irregular in nonrandom structural influences, including shape tend to have larger gaps between their macropores and is arithmetically defined as the nontouching surfaces, thus forming media of difference between the textural porosity and greater porosity. In porous such as sand- the total porosity. stone, cementation or welding of particles not The texture of the medium relates in a gen- only creates pores that are different in shape eral way to the pore-size distribution, as large from those of particulate media, but also re- particles give rise to large pores between them, duces the porosity as solid material takes up and therefore is a major influence on the soil space that would otherwise be pore space. Po- water retention curve. Additionally, the struc- rosity in such a case can easily be less than ture of the medium, especially the pervasive- 0.3, even approaching 0. Cementing material ness of aggregation, shrinkage cracks, worm- can also have the opposite effect. In many holes, etc. substantially influences water reten- soils, and organic substances par- tion. ticles together into aggregates. An individual might have a 0.35 porosity within it, Measurement of porosity but the medium as a whole has additional pore The technology of thin sections or of to- space in the form of gaps between aggregates, mographic imaging can produce a visualiza- so that φ can be 0.5 or greater. Observed po- tion of pore space and solid material in a rosities can be as great as 0.8 to 0.9 in a cross-sectional plane, as in Figure 1. The (extremely high organic matter) soil. summed area of pore space divided by total area gives the areal porosity over that plane. An analogous procedure can be followed along a line through the sample, to yield a linear po- rosity. If the medium is isotropic, either of these would numerically equal the volumetric porosity as defined above, which is more usu- ally of interest. The volume of water contained in a satu- rated sample of known volume can indicate porosity. The mass of saturated material less the oven-dry mass of the , divided by the density of water, gives the volume of water. This divided by the original sample volume gives porosity.

Figure 2. Dense packing of polydisperse An analogous method is to determine the spheres. (Adapted from Hillel, 1980, Fundamentals volume of in the pore space of a com- of soil physics, Academic Press, p. 97.) pletely dry sample. Sampling and drying of

2 REPRINT – Nimmo, J.R., 2004, Porosity and Pore Size Distribution, in Hillel, D., ed. Encyclopedia of Soils in the Environment: London, Elsevier, v. 3, p. 295-303.

the soil must be conducted so as not to com- press the soil or otherwise alter its porosity. A Pores and Pore-size Distri- pycnometer can measure the air volume in the bution pore space. A gas-tight chamber encloses the sample so that the internal gas-occupied vol- ume can be perturbed by a known amount The nature of a pore while the gas pressure is measured. This is Because soil does not contain discrete ob- typically done with a small piston attached by jects with obvious boundaries that could be a tube connection. Boyle’s law indicates the called individual pores, the precise delineation total gas volume from the change in pressure of a pore unavoidably requires artificial, sub- resulting from the volume change. This total jectively established distinctions. This con- gas volume minus the volume within the pis- trasts with soil particles, which are easily de- ton, connectors, gaps at the chamber walls, and fined, being discrete material objects with ob- any other space not occupied by soil, yields vious boundaries. The arbitrary criterion re- the total pore volume to be divided by the quired to partition pore space into individual sample volume. pores is often not explicitly stated when pores To avoid having to saturate with water or or their sizes are discussed. Because of this air, one can calculate porosity from measure- inherent arbitrariness, some scientists argue that the concepts of pore and pore size should ments of particle density ρp and ρ . From the definitions of ρ as the solid be avoided. Much valuable theory of the be- b b havior of the soil-water-air system, however, mass per total volume of soil and ρ as the p has been built on these concepts, defined using solid mass per solid volume, their ratio ρ / ρ b p widely, if not universally, accepted criteria. is the complement of φ, so that A particularly useful conceptualization takes the pore space as a collection of channels (1) φ = 1 – ρb / ρp. through which fluid can flow. The effective Often the critical source of error is in the de- width of such a channel varies along its length. termination of total soil volume, which is Pore bodies are the relatively wide portions harder to measure than the mass. This meas- and pore openings are the relatively narrow urement can be based on the of a portions that separate the pore bodies. Other minimally disturbed sample in a regular geo- anatomical metaphors are sometimes used, the metric shape, usually a cylinder. Significant wide part of a pore being the “belly” or error can result from irregularities in the actual “waist”, and the constrictive part being the shape and from unavoidable compaction. Al- “neck” or “throat”. In a medium dominated by ternatively, the measured volume can be that textural pore space, like a sand, pore bodies of the excavation from which the soil sample are the intergranular spaces of dimensions originated. This can be done using measure- typically slightly less than those of the adja- ments of a regular geometric shape, with the cent particles. At another extreme, a worm- same problems as with measurements on an hole, if it is essentially uniform in diameter extracted sample. Additional methods, such as along its length, might be considered a single the balloon or sand-fill methods, have other pore. The boundaries of such a pore are of sources of error. three types: (1) interface with solid, (2) con- striction— a plane through the locally narrow- est portion of pore space, or (3) interface with another pore (e.g. a crack or wormhole) or a hydraulically distinct region of space (e.g. the land surface).

3 REPRINT – Nimmo, J.R., 2004, Porosity and Pore Size Distribution, in Hillel, D., ed. Encyclopedia of Soils in the Environment: London, Elsevier, v. 3, p. 295-303.

This cellular, equivalent-capillary concep- tualization of pores is especially relevant to hydraulic behavior, as has been recognized for more than 70 years. The initial application was to Haines jumps, illustrated in Figure 3, still considered the basic phenomena of capillary hysteresis. The pore openings, which control the matric pressure P at which pores empty, are smaller than the pore bodies, which control the P at which pores fill. As the medium dries and P decreases, water retreats gradually as the air-water interface becomes more curved. At the narrowest part of the pore opening, this interface can no longer increase curvature by gradual amounts, so it retreats suddenly to nar- rower channels elsewhere. An analogous phe- nomenon occurs during wetting, when the de- creasing interface curvature cannot be sup- ported by the radius of the pore at its maxi- mum width. The volume that empties and fills Figure 3. Dynamics of a Haines jump. (Adapted in this way is essentially an individual pore. from Miller and Miller, 1956, J. App. Phys., v. 27, p. Not all pore space is subject to Haines 324-332.) jumps—water remains in crevices and in films (not seen in Figure 3) coating solid surfaces. Pore sizes are usually specified by an effec- Various models and theories treat this space in tive radius of the pore body or neck. The effec- different ways. By the definition above it is tive radius relates to the radius of curvature of part of a pore in addition to the volume af- the air-water interface at which Haines jumps fected by the Haines jump. occur. By capillarity this relates also to the Pores can be classified according to their matric pressures at which these occur, as dis- origin, function or other attributes. A tex- cussed in the section below. Alternative indi- tural/structural distinction is possible, analo- cators of size include the cross-sectional area gous to porosity. Intergranular pores are the or the volume of a pore, and the hydraulic ra- major portion of soil textural porosity, as dis- dius, defined as the ratio of the cross-sectional cussed above. Intragranular or dead-end pores area to circumference, or of pore volume to (if not entirely enclosed within solid) might specific surface. empty or fill with water, but without contribut- The pore-size distribution is the relative ing directly to fluid movement through the abundance of each pore size in a representative medium. Interaggregate pores, including volume of soil. It can be represented with a shrink/swell cracks, are common types of function f(r), which has a value proportional to macropores. Intraaggregate pores may be es- the combined volume of all pores whose effec- sentially equivalent to intergranular pores tive radius is within an infinitesimal range cen- within an aggregate. Biogenic pores, for ex- tered on r. Figure 4 shows examples, all of ample the channels left by decayed roots and which were derived from water retention data, the made by burrowing animals, are as explained below. Like porosity, f(r) may be another common type of macropores in soils. taken to comprise textural and structural com- ponents.

4 REPRINT – Nimmo, J.R., 2004, Porosity and Pore Size Distribution, in Hillel, D., ed. Encyclopedia of Soils in the Environment: London, Elsevier, v. 3, p. 295-303.

of segments of solid or pore along one- dimensional transects can serve similar pur- poses. As in the case of porosity, isotropy is required for assuming the equality of lineal, areal, and volumetric pore size distribution. For pore size, however, a more important problem is that when working with fewer than three dimensions, one doesn’t know what part of the pore the selected slice intersects; be- cause it does not in general go through the widest part, it underestimates the pore radius. Mathematical correction techniques are neces- sary to estimate unbiased pore body and open- ing sizes. Three-dimensional analysis is possible with impregnation techniques. In these, the soil pore space is filled with a resin or other that solidifies. After solidification, the medium is broken up and individual blobs of solid resin, actually casts of the pores, are analyzed as particles. Image-based techniques can be prohibi- Figure 4. Pore size distributions based on measured water retention. (a) Loamy soil tively tedious because enough pores must be (Schofield, R.K., 1935, The pF of the water in soil, analyzed to give an adequate statistical repre- Transactions, 3rd International Congress of Soil sentation. They can give a wealth of informa- Science: London, Murby & Co., p. 38-48). (b) Silty tion, however, on related aspects such as pore sand at two packing (Croney, D., and shape and connectivity that is not obtainable Coleman, J.D., 1954, Soil structure in relation to soil suction (pF): Journal of Soil Science, v. 5, p. otherwise. 75-84). (c) Paleosol of sandy texture from 42 More common than imaging methods are m depth, as a minimally disturbed , those based on effective capillary size. These and after disaggregation and repacking to the use data derived from fluid behavior in an un- original density (Perkins, K.S., 2003, Measurement saturated medium, usually the emptying or fill- of sedimentary interbed hydraulic properties and their hydrologic influence near the Idaho Nuclear ing of pores during soil drying or wetting Technology and Center at the Idaho (Figure 3). In other words, they use the water National Engineering and Environmental Labora- retention curve θ(P), where θ is the volumetric tory: U.S. Geological Survey Water-Resources . Because large pores fill or Investigations Report 03-4048, 18 p.). empty at P near 0, a medium that has many large pores will have a retention curve that Measurement drops rapidly to low θ at high matric poten- The most obvious and straightforward tials. Conversely, one with very fine pores will measurements of pore size are with geometric retain much water even at highly negative P, analysis of images of individual pores. This thus having a retention curve with more grad- can be done using various types of microscopy ual changes in slope. By capillary theory, the P on thin sections or other flat soil surfaces, or at which a pore empties (or fills) corresponds tomographs. Dimensions of pore bodies and to the pore opening (or body) size according to necks can be measured manually or by com- puter analysis of digitized images. The lengths

5 REPRINT – Nimmo, J.R., 2004, Porosity and Pore Size Distribution, in Hillel, D., ed. Encyclopedia of Soils in the Environment: London, Elsevier, v. 3, p. 295-303.

− 2σ cosα than the photomicrographic method, in part (2) r = P because it gives a measure of pore opening rather than body sizes, and because it relies on where σ is the surface tension and α is the dynamic accessibility of pores to the incoming contact angle. This formula can convert a fluid. In soil environmental applications, use measured θ(P) into an equivalent θ(r) curve. of the water retention curve is most common. This curve is actually a cumulative pore-size Data are more commonly available for this distribution; the water content on a drying θ(r) than for any other method. One can also ex- indicates the combined volume of all pores pect a water-based method to give better re- with opening radius less than r. Applying the sults for a water-based application (e.g. hy- fundamental theorem of calculus, the direct draulic conductivity). pore size distribution is simply the derivative: Representation dθ The basic equivalent-capillary representa- (3) f (r) = . dr tion of pore-size distribution is the function f(r) (Figure 4). Corresponding graphs of the Mercury porosimetry is analogous to the water-retention based method, but uses air as the wetting fluid, corresponding to the water, and mercury as the nonwetting fluid, corre- sponding to the air in the water-air system. Mercury is forced into the pores of dry soil incrementally, so that the relation between mercury content and mercury pressure can be recorded. Applying (2) with the appropriate values of surface tension and contact angle for mercury leads to a pore size distribution esti- mate as for the extraction of water from a wa- ter-air system. The different measurement techniques do not give exactly the same results. Emptying and filling depends on more than capillarity – different methods are affected differently by unintended influences. Contact angles, for ex- ample, are dynamic, are not likely to be at handbook values in soil, and may deviate quite differently for water and for mercury. The swelling of clays can be a major influence on a water retention curve, but should have no ef- fect with mercury. Imaging techniques are subject to some entirely different influences Figure 5. Pore size distributions obtained for an such as the chance and subjectivity involved in artificial medium using an imaging method and assessing pore bodies and openings. Figure 5 mercury intrusion (Dullien, F.A.L., and Batra, V.K., shows an example of substantially different 1970, Determination of the structure of porous me- results from different methods. The mercury dia: Industrial Engineering Chemistry, v. 62, no. 10, p. 25-53.). porosimetry method indicates smaller pores

6 REPRINT – Nimmo, J.R., 2004, Porosity and Pore Size Distribution, in Hillel, D., ed. Encyclopedia of Soils in the Environment: London, Elsevier, v. 3, p. 295-303.

cumulative size distribution can be used pothesis to break down for r of a few mm. The equivalently. Often a specific functional form experimental limit is typically about 0.5 mm. or other representational model of pore-size At either pore size extreme, where capillary distribution is useful. A normal or lognormal phenomena lose dominance, Equation (2) no distribution can be fit to the data, for example. longer applies, though it still can give r values Structural features may give the soil a bimodal corresponding to P. These values may be use- pore-size distribution, leading to several dis- ful for translating one property to another (dis- tinctive effects on water flow. Bimodal, trimo- cussed below) even though they are invalid in dal, or other multimodal forms are possible, terms of the capillary analog. and can be represented by superpositions of At intermediate values of r, sometimes f(r) the normal or lognormal forms. Self-similar or has a pronounced peak, as in Figures 4b and 5. forms of the distribution function are Such a peak is assumed to exist in many appli- also used, giving a power-law form of the cu- cations and interpretations of pore size distri- mulative pore size distribution. butions, for example normal or lognormal rep- resentations, though it does not always exist in Typical features of a pore size the measurable range of r. A peak in f(r) corre- distribution sponds to an inflection point in θ(r). The in- With the equivalent-capillary concept taken verse relation of r to P means that θ(P) is much as broadly as possible, the smallest possible more likely to have an inflection point than pore is limited to the order of a few molecular θ(r); if θ(r) has an inflection point, then θ(P) is diameters, about 1 nm. Fluid behavior in such mathematically required to have an inflection pores is likely to be dominated by interaction point, but the converse is not true. The com- with the solid material, and not necessarily de- mon case of an retention curve that shows a scribable by capillary laws or even standard wide range of slopes (with inflection point in thermodynamics. The smallest pores measured the measured range, and normally a distinct by water retention or mercury intrusion are initial-Haines-jump or air-entry effect) will typically 50 or 100 times larger than this, have a defined peak in the pore-size distribu- though with greater cost and effort, greater tion only if the middle portion of the retention magnitudes of pressure and hence smaller curve has a slope that differs markedly from measured r can be achieved. As the imputed that of the two end segments. This is fre- pore size approaches zero, in reality the water quently true for monodisperse media and for is likely to be held in thin films that coat parti- repacked samples, in which pores larger than a cle surfaces. The equivalent-capillary ap- certain r have been destroyed. For many soils, proach associates this water not with film perhaps most, f(r) does not have a peak except thicknesses but with effective radii of hypo- at r=0 or so close to 0 that it cannot be meas- thetical filled pores. Because r relates in- ured. This is especially likely for media that versely to P, the whole dry portion of the re- are macroporous, polydisperse, or that show an tention curve is contained in a very small re- air-entry effect at essentially P=0. Retention gion near r=0, where the apparent number of curves represented by a fractal or power-law pores becomes large. In the extreme case, model also are in this category. Lognormal when θ is held to remain artificially finite at an models or other representations that have a assumed residual water content as P goes to defined peak can often still be applied but with negative infinity, f(r) at r=0 is a delta function. the peak outside the measurable range. Some There is no real upper limit to pore size, models (e.g. of hysteresis and hydraulic con- though instability will cause the capillary hy- ductivity) may be unaffected by the lack of a measurable peak even though they were de-

7 REPRINT – Nimmo, J.R., 2004, Porosity and Pore Size Distribution, in Hillel, D., ed. Encyclopedia of Soils in the Environment: London, Elsevier, v. 3, p. 295-303.

rived assuming the pore size distribution re- structure of most soils adds complexity to the sembles some form of normal distribution. relation between pore size and . Large pores can be associated not only with large particles, but also with smaller particles Significance to soil and such as clays that promote aggregation and water behavior hence the existence of large interaggregate pores. With more intricate conceptualizations, Significance of porosity subdivisions of a pore size distribution can One obvious significance of porosity is that represent more detailed properties of soils, for it is an upper limit of volumetric water con- example the hysteresis of soil water retention. tent. It is similarly essential to the definition of Figure 6 shows an example in which one graph degree of saturation, θ divided by porosity. represents pore-opening and pore-body size Another significance is that within the pore distributions. Portions of the f(r) area are space, the complement to θ is gas content. shaded differently, based on criteria of how the That is, volumetric gas content equals the dif- pore body radius (rw in this diagram) relates to ference between θ and porosity. the pore opening radius (rd in this diagram) The magnitude of porosity roughly indi- and to rs (defined on the abscissa). The added cates complexity of structure, being greater for information of what fraction of pores with a greater complexity, as noted above for aggre- given opening size have a particular range of gated soil. The spatial variability of porosity is body sizes is taken to represent the essential also important, greater variability correlating quantitative basis of soil water hysteresis. with greater heterogeneity of the soil. Signifi- cant spatial variability on a small scale also Pore dynamics implies greater structural complexity, inde- Natural and artificial soil processes create pendent of the magnitude of porosity. and destroy pores, and induce changes in their size and other attributes. Table 1 lists some of Significance of pore size distri- the common effects on pore size distribution caused by routine processes. In general, if the bution soil is compacted by uniform stress, such as a A major importance of a soil’s pore size weight imposed at the land surface, it normally distribution is that it relates to other soil prop- loses large pores and gains small pores. Figure erties in a complex and useful way. It indicates complexity of structure in far more detail than porosity alone. The spatial variation of pore size is an important characteristic of the me- dium. The pore size distribution of different parts of soil is the fundamental basis for the concept of aggregates, for example. By some definitions, pore size can permit essential dis- tinctions between micropores and macropores (and mesopores, where that term is used for intermediate-size pores). The relation of pore-size to particle-size Figure 6. Hypothetical pore size distribution with subregions distinguished on the basis of pore body distribution in a randomly structured medium and opening radii and drying/wetting history is likely to be monotone: larger pores are asso- (Adapted from Nimmo, 1992, Soil Sci. Soc. Am. J., ciated with larger particles. The nonrandom v. 56, 1723-1730).

8 REPRINT – Nimmo, J.R., 2004, Porosity and Pore Size Distribution, in Hillel, D., ed. Encyclopedia of Soils in the Environment: London, Elsevier, v. 3, p. 295-303.

Table 1. Possible effects of routine soil processes on pore size distribution. Chemical activity • can constrict or obstruct pores by formation of precipitates Shrinkage • can enlarge pores by dissolution of precipi- • can enlarge macropores tates • can create new macropores • can increase or decrease interparticle cohe- • (within an aggregate) can cause intraaggregate sion, with complex effects on pore size and pores to decrease in size, or to increase in size structure if clay particles are shrinking 4b illustrates results of this type. Disturbance Swelling from irregular stresses, as during or • can decrease the size of macropores repacking, has a variety of effects on pore size, • can close macropores often with the net effect of a decrease in the • (within an aggregate) can cause intraaggregate number of large pores and an increase in the pores to increase in size, or to decrease in size number of small pores, as illustrated in Figure if clay particles are expanding 4c. Several types of processes can create pores. Though small intergranular pores are Mechanical compression seldom closed completely, some processes can • can decrease the size of macropores close macropores, in effect destroying them. • can close macropores • can break up aggregates, reducing the number of intraaggregate pores and thereby reducing Applications to soil transport the fraction of the pore space represented by properties the smallest pores Because pores are fluid conduits, their size distribution is useful for predicting hydraulic Disturbance from digging or conductivity K, as as for water retention plowing as described above. Gas and other types of • can destroy existing macropores fluid transport can be treated, though water • can create interclod macropores flow is the most common application. • can break up aggregates, reducing the number By analogy to laminar flow in tubes as of intraaggregate pores and therefore also the quantified by Poiseuille’s law, the conductance fraction of the pore space represented by the smallest pores of a single pore can be inferred to be propor- tional to the fourth power of its effective ra- Biological activity dius. This makes its hydraulic conductivity proportional to the square of its effective ra- • can create new macropores • can enlarge macropores, as by ongoing traffic dius. An estimated f(r) distribution indicates of ants or burrowing mammals the relative abundance of each conduit size, • can decrease the size of macropores, for ex- thus providing the information needed to pre- ample if they are affected by compression re- dict K. sulting from the expansion of a nearby root A K prediction based on the capillary hy- • can increase aggregation, promoting the crea- pothesis assumes that the pores that are filled tion of interaggregate macropores, and possi- bly to smaller intergranular pores within ag- at a given θ have an effective radius smaller gregates than a threshold determined from θ using the • can constrict or obstruct pores, for example by water retention relation. The portion of f(r) growth of microorganisms representing the filled pores is relevant to un- saturated K. The simplest possibility is to in- tegrate f(r) weighted by r2 over the domain

9 REPRINT – Nimmo, J.R., 2004, Porosity and Pore Size Distribution, in Hillel, D., ed. Encyclopedia of Soils in the Environment: London, Elsevier, v. 3, p. 295-303.

represented by filled pores, giving a number character in turn profoundly influences the na- proportional to K for the corresponding θ. ture and behavior of the soil. Multiplying this integration by a separately Soil porosity is fairly well standardized in determined matching factor gives the actual definition and measurement techniques. Pore predicted K. size, however, is not obvious how to define, Many specific models in the published lit- much less to measure. Yet it is central to topics erature are based on these ideas. They differ in like macropores, aggregation, fractures, soil how they treat such matters as pore length, matrix, and solute mobility. Pore size plays a connectedness, tortuosity, and the distinction key role in various proposed means of quanti- between pore opening and body dimensions. fying soil structure. It also has a major practi- Popular models include those of Mualem and cal role in the prediction of hydraulic proper- Burdine, which have been analytically com- ties. New pore size concepts, measurement bined with widely used empirical formulas for techniques, and relations to transport phenom- retention curves. ena are likely to remain a major emphasis in The pore size distribution affects solute the study of soil. convection similarly to hydraulic conductivity. Additionally it affects solute dispersion, which is expected to be greater for a broader pore- Related Articles in ESE: size distribution. It affects the sorption of sol- Aggregation: physical aspects, Capillarity, utes in a complex way. The smaller pores are Hysteresis, Isotropy and anisotropy, Macro- associated with longer residence times and pores and macropore flow, Spatial variability greater relative surface area, but most solutes of soil properties, Structure of soils, Swelling may go quickly through the large pores with and shrinking of soils, Fractal analysis of minimal opportunity to react. Interchange be- soils, Texture. tween fast-transporting and slow-transporting portions of the pore space is a vital and much- investigated aspect of solute transport in soils. Further Reading: Sometimes the terms “mobile” and “immo-

bile” are used in this context, but of course the Adamson, A.W., and Gast, A.P., 1997, Physi- distinction is not as sharp as these terms imply. cal chemistry of surfaces (Sixth ed.): New

York, Wiley, 784 p. For particle transport, many aspects are es- sentially the same as for K and solute trans- Baver, L.D., 1938, Soil permeability in rela- port. Additionally, the phenomenon of strain- tion to non-capillary porosity: Soil Science ing depends critically on the proportion of Society of America Proceedings, v. 3, p. pores smaller than a given particle size. This is 52-56. the dominant factor in some particle-transport Burdine, N.T., Gournay, L.S., and Reichertz, applications. P.P., 1950, Pore size distribution of petro- leum reservoir rocks: Transac- tions, AIME, v. 189, p. 195-204. Conclusions Childs, E.C., and Collis-George, N., 1950, The permeability of porous materials, Proceed- The characterization of pore space is a vital ings Royal Society London, Ser. A, p. 392- and fruitful aspect of soil investigation. Liquid, 405. solid and gas constituents of the soil govern Dullien, F.A.L., and Batra, V.K., 1970, De- the form and development of pores, whose termination of the structure of porous me-

10 REPRINT – Nimmo, J.R., 2004, Porosity and Pore Size Distribution, in Hillel, D., ed. Encyclopedia of Soils in the Environment: London, Elsevier, v. 3, p. 295-303.

dia: Industrial Engineering Chemistry, v. 62, no. 10, p. 25-53. Nimmo, J.R., 1997, Modeling structural influ- Haines, W.B., 1930, Studies in the physical ences on soil water retention: Soil Science properties of soil. V. The hysteresis effect Society of America Journal, v. 61, no. 3, p. in capillary properties, and the modes of 712-719. moisture distribution associated therewith: Nimmo, J.R., and Akstin, K.C., 1988, Hydrau- Journal of Agricultural Science, v. 20, p. lic conductivity of a sandy soil at low water 97-116. content after compaction by various meth- Kosugi, K., 1994, Three-parameter lognormal ods: Soil Science Society of America Jour- distribution model for soil water retention: nal, v. 52, no. 2, p. 303-310. Research, v. 30, no. 4, p. Raducu, D., Vignozzi, N., Pagliai, M., and 891-901. Petcu, G., 2002, Soil structure of tilled ho- Marshall, T.J., and Holmes, J.W., 1988, Soil rizons influenced by management practices physics (Second ed.): Cambridge, Cam- and implement geometry, in Pagliai, M., bridge University Press, 374 p. and Jones, R., eds., Sustainable land man- Miller, E.E., and Miller, R.D., 1956, Physical agement - environmental protection--a soil theory for capillary flow phenomena: Jour- physical approach: Advances in Geoecol- nal of Applied Physics, v. 27, no. 4, p. 324- ogy 35: Reiskirchen, Germany, Catena 332. Verlag, p. 149-162. Mualem, Y., 1974, A conceptual model of Ragab, R., Feyen, J., and Hillel, D., 1982, Ef- hysteresis: Water Resources Research, v. fect of the method for determining pore 10, no. 3, p. 514-520. size distribution on prediction of the hy- Mualem, Y., 1976, A new model for predict- draulic conductivity function and of infil- ing the hydraulic conductivity of unsatu- tration: Soil Science, v. 134, no. 6, p. 141- rated porous media: Water Resources Re- 145. search, v. 12, no. 3, p. 513-522.

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