View source for Porosity

{{Short description|Ratio of void volume and total volume of a porous material}}
'''Porosity''' or '''void fraction''' is a measure of the [[Void (composites)|void]] (i.e. "empty") spaces in a [[material]], and is a [[volume fraction|fraction of the volume]] of voids over the total volume, between 0 and 1, or as a [[percentage]] between 0% and 100%. Strictly speaking, some tests measure the "accessible void", the total amount of void space accessible from the [[Interface (matter)|surface]] (cf. [[closed-cell foam]]).

There are many ways to test porosity in a substance or part, such as [[industrial CT scanning]].

The term porosity is used in multiple fields including [[pharmaceutics]], [[ceramic engineering|ceramics]], [[metallurgy]], [[materials science|materials]], [[manufacturing]], [[petrophysics]], [[hydrology]], [[earth sciences]], [[soil mechanics]], [[rock mechanics]], and [[engineering]].<ref>{{cite journal |last1=Mohammadizadeh|first1=SeyedMehdi |last2=Moghaddam |first2=Mehdi Azhdary |last3=Talebbeydokhti|first3=Naser|title=Analysis of Flow in Porous Media using Combined Pressurized-Free surface Network |journal=Journal of Porous Media |date=2021 |volume=24 |issue=10 |pages=1–15 |doi=10.1615/JPorMedia.2021025407 |publisher=Begel House Inc. |s2cid=235877042 |language=en}}</ref>

== Void fraction in two-phase flow ==

In gas-liquid [[two-phase flow]], the void fraction is defined as the fraction of the flow-channel volume that is occupied by the gas phase or, alternatively, as the fraction of the cross-sectional area of the channel that is occupied by the gas phase.<ref>G.F. Hewitt, G.L. Shires, Y.V.Polezhaev (editors), "International Encyclopedia of Heat and Mass Transfer", CRC Press, 1997.</ref>

Void fraction usually varies from location to location in the flow channel (depending on the two-phase flow pattern). It fluctuates with time and its value is usually time averaged. In separated (i.e., non-[[Homogeneity and heterogeneity|homogeneous]]) flow, it is related to [[volumetric flow rate]]s of the gas and the liquid phase, and to the ratio of the velocity of the two phases (called ''[[Slip ratio (gas-liquid flow)|slip ratio]]'').

== Porosity in earth sciences and construction ==

Used in [[geology]], [[hydrogeology]], [[soil science]], and [[building science]], the porosity of a [[porous medium]] (such as [[Rock (geology)|rock]] or [[sediment]]) describes the fraction of void space in the material, where the void may contain, for example, air or water. It is defined by the [[ratio]]:

:<math>\phi = \frac{V_\mathrm{V}}{V_\mathrm{T}}</math>

where ''V''<sub>V</sub> is the volume of void-space (such as fluids) and ''V''<sub>T</sub> is the total or bulk volume of material, including the solid and void components. Both the [[Table of mathematical symbols|mathematical symbols]] <math>\phi</math> and <math>n</math> are used to denote porosity.

Porosity is a fraction between 0 and 1, typically ranging from less than 0.005 for solid [[granite]] to more than 0.5 for [[peat]] and [[clay]].

The porosity of a rock, or sedimentary layer, is an important consideration when attempting to evaluate the potential volume of [[water]] or [[hydrocarbon]]s it may contain. Sedimentary porosity is a complicated function of many factors, including but not limited to: rate of burial, depth of burial, the nature of the [[connate fluids]], the nature of overlying sediments (which may impede fluid expulsion). One commonly used relationship between porosity and depth is the decreasing [[exponential function]] given by the Athy (1930) equation:<ref>Athy L.F., 1930. Density, porosity and compactation of sedimentary rocks, ''Bull. Amer. Assoc. Petrol. Geol.'' v. 14, pp. 1-24.</ref>

: <math>\phi(z) = \phi_0 e^{-kz}\,</math>

where, <math>\phi(z)</math> is the porosity of the sediment at a given depth (<math>z</math>) (m), <math>\phi_0</math> is the initial porosity of the sediment at the surface of soil (before its burial), and <math>k</math> is the compaction coefficient (m<sup>−1</sup>). The letter <math>e</math> with a negative exponent denotes the decreasing exponential function. The porosity of the sediment exponentially decreases with depth, as a function of its compaction. 

A value for porosity can alternatively be calculated from the [[bulk density]] <math>\rho_{\text{bulk}}</math>, saturating [[fluid density]] <math>\rho_{\text{fluid}}</math> and [[particle density (packed density)|particle density]] <math>\rho_{\text{particle}}</math>:
:<math>\phi = \frac{\rho_{\text{particle}} - \rho_{\text{bulk}}}{\rho_{\text{particle}} - \rho_{\text{fluid}}}</math>

If the void space is filled with air, the following simpler form may be used:
:<math>\phi = 1-\frac{\rho_{\text{bulk}}}{\rho_{\text{particle}}}</math>
A mean normal particle density can be taken as approximately 2.65&nbsp;g/cm<sup>3</sup> ([[silica]], siliceous sediments or aggregates), or 2.70&nbsp;g/cm<sup>3</sup> ([[calcite]], carbonate sediments or aggregates), although a better estimation can be obtained by examining the [[Petrology|lithology]] of the particles.

===Porosity and hydraulic conductivity===

Porosity can be proportional to [[hydraulic conductivity]]; for two similar [[sand]]y [[aquifer]]s, the one with a higher porosity will typically have a higher [[hydraulic conductivity]] (more open area for the flow of water), but there are many complications to this relationship. The principal complication is that there is not a direct proportionality between porosity and hydraulic conductivity but rather an inferred proportionality. There is a clear proportionality between pore throat radii and hydraulic conductivity. Also, there tends to be a proportionality between pore throat radii and pore volume. If the proportionality between pore throat radii and porosity exists then a proportionality between porosity and hydraulic conductivity may exist. However, as grain size or sorting decreases the proportionality between pore throat radii and porosity begins to fail and therefore so does the proportionality between porosity and hydraulic conductivity. For example: clays typically have very low hydraulic conductivity (due to their small pore throat radii) but also have very high porosities (due to the structured nature of [[clay minerals]]), which means clays can hold a large volume of water per volume of bulk material, but they do not release water rapidly and therefore have low hydraulic conductivity.

===Sorting and porosity===

[[Image:Well sorted vs poorly sorted porosity.svg|thumb|right|200px|Effects of sorting on [[alluvial]] porosity. Black represents solids, blue represents pore space.]]
[[Particle size|Well sorted]] (grains of approximately all one size) materials have higher porosity than similarly sized poorly sorted materials (where smaller particles fill the gaps between larger particles). The graphic illustrates how some smaller grains can effectively fill the pores (where all water flow takes place), drastically reducing porosity and hydraulic conductivity, while only being a small fraction of the total volume of the material. For tables of common porosity values for [[earth materials]], see the "further reading" section in the [[Hydrogeology]] article.

===Porosity of rocks===

Consolidated rocks (e.g., [[sandstone]], [[shale]], [[granite]] or [[limestone]]) potentially have more complex "dual" porosities, as compared with [[Alluvium|alluvial sediment]]. This can be split into connected and unconnected porosity. Connected porosity is more easily measured through the volume of gas or liquid that can flow into the rock, whereas fluids cannot access unconnected pores.

Porosity is the ratio of pore volume to its total volume. Porosity is controlled by: rock type, pore distribution, cementation, [[Diagenesis|diagenetic history]] and composition. Porosity is not controlled by grain size, as the volume of between-grain space is related only to the method of grain packing.

Rocks normally decrease in porosity with age and depth of burial. [[Tertiary]] age [[Gulf Coast]] sandstones are in general more porous than [[Cambrian]] age sandstones. There are exceptions to this rule, usually because of the depth of burial and thermal history.

===Porosity of soil===
{{Main|Porosity of soil}}

Porosity of surface soil typically decreases as particle size increases. This is due to soil [[Aggregate (geology)|aggregate]] formation in finer textured surface soils when subject to [[soil life|soil biological]] processes. Aggregation involves particulate adhesion and higher resistance to compaction. Typical bulk density of sandy soil is between 1.5 and 1.7&nbsp;g/cm<sup>3</sup>. This calculates to a porosity between 0.43 and 0.36. Typical bulk density of clay soil is between 1.1 and 1.3&nbsp;g/cm<sup>3</sup>. This calculates to a porosity between 0.58 and 0.51. This seems counterintuitive because clay soils are termed ''heavy'', implying ''lower'' porosity. Heavy apparently refers to a gravitational [[moisture content]] effect in combination with terminology that harkens back to the relative force required to pull a [[tillage]] implement through the clayey soil at field moisture content as compared to sand.

Porosity of subsurface soil is lower than in surface soil due to compaction by gravity. Porosity of 0.20 is considered normal for unsorted gravel size material at depths below the [[bioturbation|biomantle]]. Porosity in finer material below the aggregating influence of [[pedogenesis]] can be expected to approximate this value.

Soil porosity is complex. Traditional models regard porosity as continuous. This fails to account for anomalous features and produces only approximate results. Furthermore, it cannot help model the influence of [[environmental factor]]s which affect pore geometry. A number of more complex models have been proposed, including [[fractal]]s, [[liquid bubble|bubble]] theory, [[Fracture|cracking]] theory, [[Boolean model (probability theory)|Boolean]] grain process, packed sphere, and numerous other models. The [[characterisation of pore space in soil]] is an associated concept.

===Types of geologic porosities===
;Primary porosity: The main or original porosity system in a [[rock (geology)|rock]] or unconfined [[alluvium|alluvial deposit]].
;Secondary porosity: A subsequent or separate porosity system in a rock, often enhancing overall porosity of a rock. This can be a result of chemical leaching of minerals or the generation of a fracture system. This can replace the primary porosity or coexist with it (see dual porosity below).
;Fracture porosity: This is porosity associated with a fracture system or faulting. This can create secondary porosity in rocks that otherwise would not be reservoirs for hydrocarbons due to their primary porosity being destroyed (for example due to depth of burial) or of a rock type not normally considered a reservoir (for example igneous intrusions or metasediments).
;Vuggy porosity: This is secondary porosity generated by dissolution of large features (such as [[macrofossil]]s) in [[carbonate rock]]s leaving large holes, [[vug]]s, or even [[cave]]s.
;[[Effective porosity]] (also called ''open porosity''): Refers to the fraction of the total volume in which [[Fluid dynamics|fluid flow]] is effectively taking place and includes [[catenary]] and dead-end (as these pores cannot be flushed, but they can cause fluid movement by release of pressure like gas expansion<ref>[http://www.epgeology.com/petrophysics-f11/what-the-difference-between-secondary-primary-porosity-t252.html Effective and Ineffective Porosity] or [http://www.epgeology.com/petrophysics-f23/total-and-effective-porosity-explained-t5778.html Total and Effective Porosity Explained] at [http://www.epgeology.com/ E&P Geology.com] {{Webarchive|url=https://web.archive.org/web/20120313183559/http://www.epgeology.com/petrophysics-f11/what-the-difference-between-secondary-primary-porosity-t252.html |date=2012-03-13 }}</ref>) pores and excludes closed pores (or non-connected cavities). This is very important for groundwater and petroleum flow, as well as for solute transport.
;Ineffective porosity (also called ''closed porosity''): Refers to the fraction of the total volume in which fluids or gases are present but in which [[Fluid dynamics|fluid flow]] can not effectively take place and includes the closed pores. Understanding the morphology of the porosity is thus very important for groundwater and petroleum flow.
;Dual porosity: Refers to the conceptual idea that there are two overlapping reservoirs which interact. In fractured rock aquifers, the rock mass and fractures are often simulated as being two overlapping but distinct bodies. Delayed yield, and leaky aquifer flow solutions are both mathematically similar solutions to that obtained for dual porosity; in all three cases water comes from two mathematically different reservoirs (whether or not they are physically different).
;[[Macropore|Macroporosity]]: In solids (i.e. excluding aggregated materials such as soils), the term 'macroporosity' refers to pores greater than 50&nbsp;[[nanometer|nm]] in diameter. Flow through macropores is described by bulk diffusion.
;[[Mesoporous material|Mesoporosity]]: In solids (i.e. excluding aggregated materials such as soils), the term 'mesoporosity' refers to pores greater than 2&nbsp;nm and less than 50&nbsp;nm in diameter. Flow through mesopores is described by Knudsen diffusion.
;[[Microporous material|Microporosity]]: In solids (i.e. excluding aggregated materials such as soils), the term 'microporosity' refers to pores smaller than 2&nbsp;nm in diameter. Movement in micropores is activated by diffusion.

==Porosity of fabric or aerodynamic porosity==
{{further|Fiber volume ratio}}
The ratio of holes to solid that the wind "sees". [[Aerodynamic]] porosity is less than visual porosity, by an amount that depends on the constriction of holes.

==Die casting porosity==
Casting porosity is a consequence of one or more of the following: gasification of contaminants at molten-metal temperatures; shrinkage that takes place as molten metal solidifies; and unexpected or uncontrolled changes in temperature or humidity.

While porosity is inherent in die casting manufacturing, its presence may lead to component failure where pressure integrity is a critical characteristic. Porosity may take on several forms from interconnected micro-porosity, folds, and inclusions to macro porosity visible on the part surface. The end result of porosity is the creation of a leak path through the walls of a casting that prevents the part from holding pressure. Porosity may also lead to out-gassing during the painting process, leaching of plating acids and tool chatter in machining pressed metal components.<ref>{{cite web|title=How to Fix Die Casting Porosity?|url=https://www.godfreywing.com/blog/how-to-fix-die-casting-porosity|website=Godfrey & Wing}}</ref>

==Measuring porosity==
[[File:Porosity thin section GP.jpg|thumb|Optical method of measuring porosity: [[thin section]] under gypsum plate shows porosity as purple color, contrasted with carbonate grains of other colors. [[Pleistocene]] [[eolianite]] from [[San Salvador Island]], Bahamas. Scale bar 500&nbsp;[[μm]].]]
Several methods can be employed to measure porosity:
* Direct methods (determining the bulk volume of the porous sample, and then determining the volume of the skeletal material with no pores (pore volume&nbsp;= total volume&nbsp;− material volume).
* Optical methods (e.g., determining the area of the material versus the area of the pores visible under the microscope). The "areal" and "volumetric" porosities are equal for porous media with random structure.<ref name="Dul"/>
* Computed tomography method (using [[industrial CT scanning]] to create a 3D rendering of external and internal geometry, including voids. Then implementing a defect analysis utilizing computer software)
* [[Imbibition]] methods,<ref name="Dul"/> i.e., immersion of the porous sample, under vacuum, in a fluid that preferentially wets the pores.
** Water saturation method (pore volume&nbsp;= total volume of water&nbsp;− volume of water left after soaking).
* Water evaporation method (pore volume&nbsp;= (weight of saturated sample&nbsp;− weight of dried sample)/density of water)
* Mercury intrusion [[porosimetry]] (several non-mercury intrusion techniques have been developed due to toxicological concerns, and the fact that mercury tends to form amalgams with several metals and alloys).
* Gas expansion method.<ref name="Dul">F.A.L. Dullien, "Porous Media. Fluid Transport and Pore Structure", [[Academic Press]], 1992.</ref> A sample of known bulk volume is enclosed in a container of known volume. It is connected to another container with a known volume which is evacuated (i.e., near vacuum pressure). When a valve connecting the two containers is opened, gas passes from the first container to the second until a uniform pressure distribution is attained. Using [[ideal gas]] law, the volume of the pores is calculated as
:<math>V_V = V_T-V_a-V_b {P_2 \over {P_2-P_1}}</math>,
where
:V<sub>V</sub> is the effective volume of the pores,
:V<sub>T</sub> is the bulk volume of the sample,
:V<sub>a</sub> is the volume of the container containing the sample,
:V<sub>b</sub> is the volume of the evacuated container,
:P<sub>1</sub> is the initial pressure in the initial pressure in volume V<sub>a</sub> and V<sub>V</sub>, and
:P<sub>2</sub> is final pressure present in the entire system.
:The porosity follows straightforwardly by its proper definition
:<math>\phi = \frac{V_V}{V_T}</math>.
:Note that this method assumes that gas communicates between the pores and the surrounding volume. In practice, this means that the pores must not be closed cavities.
* Thermoporosimetry and cryoporometry. A small crystal of a liquid melts at a lower temperature than the bulk liquid, as given by the [[Gibbs–Thomson effect|Gibbs-Thomson equation]]. Thus if a liquid is imbibed into a porous material, and frozen, the melting temperature will provide information on the pore-size distribution. The detection of the melting can be done by sensing the transient heat flows during phase-changes using [[differential scanning calorimetry]] – (DSC thermoporometry),<ref>{{Cite journal | title = A new method for the simultaneous determination of the size and the shape of pores: The Thermoporometry
 | journal = Thermochimica Acta
 | volume = 21
 | pages = 59–88
 | year = 1977
 | publisher = Elsevier Scientific Publishing Company, Amsterdam
 | last1 = Brun | first1 = M.
 | last2 = Lallemand | first2 = A.
 | last3 = Quinson | first3 = J-F.
 | last4 = Eyraud | first4 = C. | issue = 1
 | doi = 10.1016/0040-6031(77)85122-8 | bibcode = 1977TcAc...21...59B
 }}</ref> measuring the quantity of mobile liquid using [[nuclear magnetic resonance]] – (NMR cryoporometry)<ref>{{Cite journal
 | title = Nuclear Magnetic Resonance Cryoporometry
 | journal = Phys. Rep.
 | year = 2008
 | volume = 461
 | issue = 1
 | pages = 1–36
 | first1 = J. | last1 = Mitchell
 | first2 = J. Beau W. | last2 = Webber
 | first3 = J.H. | last3 = Strange
 | doi = 10.1016/j.physrep.2008.02.001
 | bibcode=2008PhR...461....1M
 | url = http://kar.kent.ac.uk/13467/6/NMRcryov10c_BibTexRefs_figs_ed.pdf
 }}</ref> or measuring the amplitude of [[neutron scattering]] from the imbibed crystalline or liquid phases – (ND cryoporometry).<ref>{{Cite journal
 | title = Neutron Diffraction Cryoporometry – a measurement technique for studying mesoporous materials and the phases of contained liquids and their crystalline forms
 | journal = Nucl. Instrum. Methods A
 | year = 2008
 | volume = 586
 | pages = 356–66
 | doi = 10.1016/j.nima.2007.12.004
 | last1 = Webber | first1 = J. Beau W.
 | last2 = Dore | first2 = John C.
 | issue = 2
 | bibcode=2008NIMPA.586..356W
| s2cid = 28074381
 | url = http://kar.kent.ac.uk/13471/7/NDC_2007-10-31.pdf
 }}</ref>

==See also==
* [[Void ratio]]
* [[Petroleum geology]]
* [[Poromechanics]]
* [[Bulk density]]
* [[Particle density (packed density)]]
* [[Packing density]]
* [[Void (composites)]]
* [[Coherent diffraction imaging]]

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== Footnotes ==
{{Reflist}}

==External links==
* [http://perminc.com/resources/fundamentals-of-fluid-flow-in-porous-media/chapter-2-the-porous-medium/porosity/ Absolute Porosity & Effective Porosity Calculations]
* [https://geology.buzz/threads/porosity.104/ Geology Buzz: Porosity]

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[[Category:Aquifers]]
[[Category:Hydrogeology]]
[[Category:Porous media]]
[[Category:Soil physics]]
[[Category:Soil mechanics]]
[[Category:Physical quantities]]