Intensive and extensive properties: Difference between revisions

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{{Short description|Properties independent of system size, and proportional to system size}}

{{Refimprove|date=April 2010}}

{{Distinguish|Intrinsic and extrinsic properties}}

[[Physical properties]] of materials and [[system]]s are often described as '''intensive and extensive properties'''. This classification relates to the dependency of the properties upon the size or extent of the system or object in question.

{{Thermodynamics|expanded=sysprop}}

[[Physical property|Physical]] or [[Chemical property|chemical]] [[Material property|properties of materials]] and [[system]]s can often be categorized as being either '''intensive''' or '''extensive''', according to how the property changes when the size (or extent) of the system changes.

The distinction is based on the concept that smaller, non-interacting identical subdivisions of the system may be identified so that the property of interest does or does not change when the system is divided or combined.

The terms "intensive and extensive quantities" were introduced into physics by German mathematician [[Georg Helm]] in 1898, and by American physicist and chemist [[Richard C. Tolman]] in 1917.<ref name="Redlich" /><ref name="Tolman">{{cite journal |author=Tolman, Richard C. |year=1917 |title=The Measurable Quantities of Physics |journal=Phys. Rev. |volume=9 |issue=3 |pages=237–253}}[https://archive.org/details/physicalreview18univgoog/page/n250/mode/2up]</ref>

According to [[International Union of Pure and Applied Chemistry]] (IUPAC), an '''intensive property''' or '''intensive quantity''' is one whose magnitude is independent of the size of the system.<ref>{{GoldBookRef|file=I03074|title=Intensive quantity}}</ref>

An '''intensive property''' is a '''bulk property''', meaning that it is a [[physical property]] of a system that does not depend on the system size or the amount of material in the system. Examples of intensive properties include temperature, refractive index, density, and hardness of an object. When a diamond is cut, the pieces maintain their intrinsic hardness (until their size reaches a few atoms thick).

An intensive property is not necessarily homogeneously distributed in space; it can vary from place to place in a body of matter and radiation. Examples of intensive properties include [[temperature]], ''T''; [[refractive index]], ''n''; [[density]], ''ρ''; and [[hardness]], ''η''.

By contrast, an '''extensive property''' or '''extensive quantity''' is one whose magnitude is additive for subsystems.<ref>{{GoldBookRef|file=E02281|title=Extensive quantity}}</ref>

By contrast, an '''extensive property''' is one that is additive for independent, noninteracting subsystems.<ref name=IUPAC>[http://media.iupac.org/publications/books/gbook/IUPAC-GB3-2ndPrinting-Online-22apr2011.pdf IUPAC Green Book] Quantities, Units and Symbols in Physical Chemistry (3rd edn. 2007), page 6 (page 20 of 250 in PDF file)</ref> The property is proportional to the amount of material in the system. For example, both the mass and the volume of a diamond are directly proportional to the amount that is left after cutting it from the raw mineral. Mass and volume are extensive properties, but hardness is intensive.

Examples include [[mass]], [[volume]] and [[Gibbs free energy|Gibbs energy]].<ref name="IUPACgreen">{{cite book | url=http://media.iupac.org/publications/books/gbook/IUPAC-GB3-2ndPrinting-Online-22apr2011.pdf | title=IUPAC Green Book | publisher=IUPAC and RSC Publishing | author=Cohen, E. R. | author-link=Quantities, Units and Symbols in Physical Chemistry | year=2007 | ___location=Cambridge | pages=6 (20 of 250 in PDF file) | isbn=978-0-85404-433-7 | edition=3rd|display-authors=etal}}</ref>

Not all properties of matter fall into these two categories. For example, the square root of the volume is neither intensive nor extensive.<ref name=Redlich/> If a system is doubled in size by juxtaposing a second identical system, the value of an intensive property equals the value for each subsystem and the value of an extensive property is twice the value for each subsystem. However the property √V is instead multiplied by √2 .

The ratio of two extensive properties is scale-invariant, and is therefore an intensive property. For example, when gravity may be assumed constant, the ratio of the extensive properties mass and volume, the density, is an intensive property.

The distinction between intensive and extensive properties has some theoretical uses. For example, in thermodynamics, the state of a simple compressible system is completely specified by two independent, intensive properties, along with one extensive property, such as mass. Other intensive properties are derived from those two intensive variables.

This terminology of intensive and extensive properties was introduced by [[Richard C. Tolman]] in 1917.<ref name=Redlich/>

==Intensive properties==

An intensive property is a [[physical quantity]] whose value does not depend on the amount of the substance for which it iswas measured. ForThe example,most theobvious [[temperature]]intensive ofquantities aare system in thermal equilibrium is the same as the temperatureratios of anyextensive part of itquantities. If the system is divided the temperature of each subsystem is identical. The same applies to the [[density]] ofIn a homogeneous system; ifdivided theinto systemtwo is divided in halfhalves, theall massits andextensive the volume changeproperties, in theparticular identicalits ratiovolume and theits density remains unchanged. Additionallymass, theare boilingdivided pointinto oftwo ahalves. substanceAll is another example of anits intensive property.properties, Forsuch example,as the boilingmass pointper forvolume water(mass isdensity) 100&nbsp;°Cor atvolume aper pressure of onemass ([[atmospherespecific (unit)|atmospherevolume]]), amust factremain whichthe remainssame truein regardlesseach of quantityhalf.

The [[temperature]] of a system in thermal equilibrium is the same as the temperature of any part of it, so temperature is an intensive quantity. If the system is divided by a wall that is permeable to heat or to matter, the temperature of each subsystem is identical. Additionally, the boiling temperature of a substance is an intensive property. For example, the boiling temperature of water is 100&nbsp;°C at a pressure of one [[atmosphere (unit)|atmosphere]], regardless of the quantity of water remaining as liquid.

According to the [[state postulate]], for a sufficiently simple thermodynamic system, only two independent intensive variables are needed to fully specify the entire state of a system. Other intensive properties can be derived from the two known values.

===Examples===

Some intensive properties, such as [[viscosity]], are [[empirical]] [[macroscopic]] [[quantity|quantities]] <!-- was: "statistical in nature" --> and are not relevant to extremely small systems.

Examples of intensive properties include:<ref name=IUPACgreen /><ref name=Tolman /><ref name=Redlich />

{{div col|colwidth=22em}}

* charge density, ''ρ'' (or ''ne'')

* [[chemical potential]], ''μ''

* [[color]]<ref name="Chang">{{cite book | title=Chemistry | publisher=McGraw-Hill Education |author1=Chang, R. |author2=Goldsby, K. | year=2015 | pages=312 | isbn=978-0078021510 | edition=12th}}</ref>

* [[concentration]], ''c''

* energy density, ''ρ''

* [[permeability (electromagnetism)|magnetic permeability]], ''μ''

* mass [[density]], ''ρ'' (or [[specific gravity]])

* [[melting point]] and [[boiling point]]<ref name=BrownLeMay />

* [[molality]], ''m'' or ''b''

* [[molar mass]], ''M''

* [[molar volume]], ''V''{{sub|m}}

* [[pressure]], ''p''

* [[refractive index]]

* [[Electrical resistivity and conductivity|specific conductance]] (or electrical conductivity)

* [[specific heat capacity]], ''c_p''

* [[specific internal energy]], ''u''

* [[specific rotation]], [''α'']

* [[specific volume]], ''v''

* [[standard reduction potential]],<ref name="BrownLeMay">{{cite book | title=Chemistry: The Central Science | publisher=Prentice Hall |author1=Brown, T. E. |author2=LeMay, H. E. |author3=Bursten, B. E. |author4=Murphy, C. |author5=Woodward |author6=P. |author7=Stoltzfus, M. E. | year=2014 |isbn=978-0321910417 | edition=13th}}</ref> ''E°''

* [[surface tension]]

* [[temperature]], ''T''

* [[thermal conductivity]]

* [[velocity]] ''v''

* [[viscosity]]

{{div col end}}See [[List of materials properties]] for a more exhaustive list specifically pertaining to materials.

===Combined intensiveExtensive properties===

An extensive property is a physical quantity whose value is proportional to the size of the [[system]] it describes,<ref>{{cite book |last1=Engel |first1=Thomas |last2=Reid |first2=Philip |title=Physical Chemistry |date=2006 |publisher=Pearson / Benjamin Cummings |isbn=0-8053-3842-X |page=6 |quote=A variable ... proportional to the size of the system is referred to as an extensive variable.}}</ref> or to the quantity of matter in the system. For example, the mass of a sample is an extensive quantity; it depends on the amount of substance. The related intensive quantity is the density which is independent of the amount. The density of water is approximately 1g/mL whether you consider a drop of water or a swimming pool, but the mass is different in the two cases.

There are four properties in any thermodynamic system, two are intensive and two are extensive.

Dividing one extensive property by another extensive property gives an intensive property—for example: [[mass]] (extensive) divided by [[Volume (thermodynamics)|volume]] (extensive) gives [[density]] (intensive).<ref>{{cite book |last1=Laidler |first1=Keith J. |last2=Meiser |first2=John H. |title=Physical Chemistry |date=1982 |publisher=Benjamin/Cummings |isbn=0-8053-5682-7 |page=6}}</ref>

If the set of parameters, <math>\{a_i\}</math>, are intensive properties and another set, <math>\{A_j\}</math>, are extensive properties, then the function <math>F(\{a_i\},\{A_j\})</math> is an intensive property if for all <math>\alpha</math>,

Any extensive quantity E for a sample can be divided by the sample's volume, to become the "E density" for the sample;

:<math>F(\{\alpha a_i\},\{A_j\}) = F(\{a_i\},\{A_j\}).\,</math>

similarly, any extensive quantity "E" can be divided by the sample's mass, to become the sample's "specific E";

extensive quantities "E" which have been divided by the number of moles in their sample are referred to as "molar E".

=== Examples ===

It follows, for example, that the [[ratio]] of two extensive properties is an intensive property - density (intensive) is equal to mass (extensive) divided by volume (extensive).

Examples of extensive properties include:<ref name="IUPACgreen" /><ref name="Tolman" /><ref name="Redlich" />

{{div col|colwidth=22em}}

* [[Number of moles|amount of substance]], ''n''

* [[enthalpy]], ''H''

* [[entropy]], ''S''

* [[Gibbs energy]], ''G''

* [[heat capacity]], ''C_p''

* [[Helmholtz energy]], ''A'' or ''F''

* [[internal energy]], ''U''

* [[spring stiffness]], ''K''

* [[mass]], ''m''

* [[Volume (thermodynamics)|volume]], ''V''

{{div col end}}

==Conjugate quantities==

===Examples===

In thermodynamics, some extensive quantities measure amounts that are conserved in a thermodynamic process of transfer. They are transferred across a wall between two thermodynamic systems or subsystems. For example, species of matter may be transferred through a semipermeable membrane. Likewise, volume may be thought of as transferred in a process in which there is a motion of the wall between two systems, increasing the volume of one and decreasing that of the other by equal amounts.

Examples of intensive properties include:

{{colbegin|3}}

* [[chemical potential]]

* [[concentration]]

* [[density]] (or [[specific gravity]])

* [[ductility]]

* [[Elasticity (physics)|elasticity]]

* [[electrical resistivity]]

* [[hardness]]

* [[magnetic field]]

* [[magnetization]]

* [[malleability]]

* [[melting point]] and [[boiling point]]

* [[molar absorptivity]]

* [[pressure]]

* [[specific energy]]

* [[specific heat capacity]]

* [[specific volume]]

* spectral absorption maxima (in [[solution]])

* [[temperature]]

* [[viscosity]]

{{colend}}

On the other hand, some extensive quantities measure amounts that are not conserved in a thermodynamic process of transfer between a system and its surroundings. In a thermodynamic process in which a quantity of energy is transferred from the surroundings into or out of a system as heat, a corresponding quantity of entropy in the system respectively increases or decreases, but, in general, not in the same amount as in the surroundings. Likewise, a change in the amount of electric polarization in a system is not necessarily matched by a corresponding change in electric polarization in the surroundings.

==Extensive properties==

An extensive property is defined by the [[IUPAC Green Book]] as a physical quantity which is the sum of the properties of separate noninteracting subsystems that compose the entire system.<ref name=IUPAC/> The value of such an additive property is proportional to the size of the [[system]] it describes, or to the quantity of matter in the system. Taking on the example of melting ice, the amount of heat required to melt ice is an extensive property. The amount of heat required to melt one ice cube would be much less than the amount of heat required to melt an iceberg, so it is dependent on the quantity.

In a thermodynamic system, transfers of extensive quantities are associated with changes in respective specific intensive quantities. For example, a volume transfer is associated with a change in pressure. An entropy change is associated with a temperature change. A change in the amount of electric polarization is associated with an electric field change. The transferred extensive quantities and their associated respective intensive quantities have dimensions that multiply to give the dimensions of energy. The two members of such respective specific pairs are mutually conjugate. Either one, but not both, of a conjugate pair may be set up as an independent state variable of a thermodynamic system. Conjugate setups are associated by [[Legendre transformation]]s.

Extensive properties are the counterparts of intensive properties, which are intrinsic to a particular subsystem. Dividing one type of extensive property by a different type of extensive property will in general give an intensive value. For example, [[mass]] (extensive) divided by [[Volume (thermodynamics)|volume]] (extensive) gives [[density]] (intensive).

===Combined extensiveComposite properties===

The ratio of two extensive properties of the same object or system is an intensive property. For example, the ratio of an object's mass and volume, which are two extensive properties, is density, which is an intensive property.<ref name="Canagaratna">{{cite journal | title=Intensive and Extensive: Underused Concepts | author=Canagaratna, Sebastian G. | journal=J. Chem. Educ. | year=1992 | volume=69 | issue=12 | pages=957–963 | doi=10.1021/ed069p957|bibcode = 1992JChEd..69..957C }}</ref>

If a set of parameters <math>\{a_i\}</math> are intensive properties and another set <math>\{A_j\}</math> are extensive properties, then the function <math>F(\{a_i\},\{A_j\})</math> is an extensive property if for all <math>\alpha</math>,

More generally properties can be combined to give new properties, which may be called derived or composite properties. For example, the base quantities<ref>{{GoldBookRef|file=B00609|title=Base quantity}}</ref> mass and volume can be combined to give the derived quantity<ref>{{GoldBookRef|file=D01614|title=Derived quantity}}</ref> density. These composite properties can sometimes also be classified as intensive or extensive. Suppose a composite property <math>F</math> is a function of a set of intensive properties <math>\{a_i\}</math> and a set of extensive properties <math>\{A_j\}</math>, which can be shown as <math>F(\{a_i\},\{A_j\})</math>. If the size of the system is changed by some scaling factor, <math>\lambda</math>, only the extensive properties will change, since intensive properties are independent of the size of the system. The scaled system, then, can be represented as <math>F(\{a_i\},\{\lambda A_j\})</math>.

:<math>F(\{a_i\},\{\alpha A_j\})=\alpha F(\{a_i\},\{A_j\}).\,</math>

Intensive properties are independent of the size of the system, so the property F is an intensive property if for all values of the scaling factor, <math>\lambda</math>,

Thus, extensive properties are [[homogeneous function]]s (of degree 1) with respect to <math>\{A_j\}</math>. It follows from [[Euler's homogeneous function theorem]] that

:<math>F(\{a_i\},\{\lambda A_j\}) =\sum_j A_j \leftF(\frac{a_i\partial F},\{A_j\partial A_j}\right).\,</math>

(This is equivalent to saying that intensive composite properties are [[homogeneous function]]s of degree 0 with respect to <math>\{A_j\}</math>.)

where the [[partial derivative]] is taken with all parameters constant except <math>A_j</math>. The converse is also true - any function which obeys the above relationship will be extensive.{{Citation needed|date=February 2009}}

It follows, for example, that the [[ratio]] of two extensive properties is an intensive property. To illustrate, consider a system having a certain mass, <math>m</math>, and volume, <math>V</math>. The density, <math>\rho</math> is equal to mass (extensive) divided by volume (extensive): <math>\rho=\frac{m}{V}</math>. If the system is scaled by the factor <math>\lambda</math>, then the mass and volume become <math>\lambda m</math> and <math>\lambda V</math>, and the density becomes <math>\rho=\frac{\lambda m}{\lambda V}</math>; the two <math>\lambda</math>s cancel, so this could be written mathematically as <math>\rho (\lambda m, \lambda V) = \rho (m, V)</math>, which is analogous to the equation for <math>F</math> above.

===Examples===

Examples of extensive properties include{{Citation needed|date=February 2009}}:

{{colbegin|3}}

* [[energy]]

* [[entropy]]

* [[Gibbs energy]]

* [[length]]

* [[mass]]

* [[particle number]]

* [[momentum]]

* [[number of moles]]

* [[volume (thermodynamics)|volume]]

* [[magnetic moment]]

* [[electrical charge]]

* [[weight]]

{{colend}}

The property <math>F</math> is an extensive property if for all <math>\lambda</math>,

==Related extensive and intensive properties==

{{Thermodynamics|cTopic=[[List of thermodynamic properties|System properties]]}}

{{see also|List of thermodynamic properties}}

Although not true for all physical properties, some properties have corresponding extensive and intensive analogs, many of which are [[Thermodynamic property|thermodynamic properties]]. Examples of such extensive thermodynamic properties, that are dependent on the size of the [[thermodynamic system]] in question, include volume, internal energy, enthalpy, entropy, Gibbs free energy, Helmholtz free energy, and heat capacity (in the sense of [[thermal mass]]). The symbols of these extensive thermodynamic properties shown here are [[capital letter]]s.

:<math>F(\{a_i\},\{\lambda A_j\})=\lambda F(\{a_i\},\{A_j\}).\,</math>

For homogeneous substances, these extensive thermodynamic properties each have corresponding intensive thermodynamic properties, which are expressed on a per mass or volume basis. The name is usually prefixed with the adjective ''specific'' to indicate that they are bulk properties, valid at any ___location (smaller subdivision) in a thermodynamic system. They may be dependent on other conditions at any point, such as temperature, pressure, and material composition, but are not considered dependent on the size of a thermodynamic system or on the amount of material in the system.

(This is equivalent to saying that extensive composite properties are [[homogeneous function]]s of degree 1 with respect to <math>\{A_j\}</math>.) It follows from [[Euler's homogeneous function theorem]] that

Specific volume is volume per mass, the [[Multiplicative inverse|reciprocal]] of [[density]] which equals mass per volume.

{| class="wikitable" style="width: 44em;"

:<math>F(\{a_i\},\{A_j\})=\sum_j A_j \left(\frac{\partial F}{\partial A_j}\right),</math>

|+ Corresponding extensive and intensive thermodynamic properties

where the [[partial derivative]] is taken with all parameters constant except <math>A_j</math>.<ref name="Alberty">{{cite journal | url=http://www.iupac.org/publications/pac/2001/pdf/7308x1349.pdf | title=Use of Legendre transforms in chemical thermodynamics | author=Alberty, R. A. | journal=Pure Appl. Chem. | year=2001 | volume=73 | issue=8 | pages=1349–1380 | doi=10.1351/pac200173081349| s2cid=98264934 }}</ref> This last equation can be used to derive thermodynamic relations.

==={{anchor|"Specific" properties}} Specific properties===

{{main|Specific quantity}}

{{Further|List of thermodynamic properties}}

A ''specific'' property is the intensive property obtained by dividing an extensive property of a system by its mass. For example, heat capacity is an extensive property of a system. Dividing heat capacity, <math>C_p</math>, by the mass of the system gives the specific heat capacity, <math>c_p</math>, which is an intensive property. When the extensive property is represented by an upper-case letter, the symbol for the corresponding intensive property is usually represented by a lower-case letter. Common examples are given in the table below.<ref name="IUPACgreen" />

{| class="wikitable" style="text-align: center;"

|+ Specific properties derived from extensive properties

|-

!style scope="width:15em;col" | '''Extensive'''<br />'''property'''

!style scope="width:4em;col" | '''Symbol'''

!style scope="width:8em;col" | '''SI units'''

!style scope="width:20em;col" | '''Intensive''' (specific)<br />'''property**'''

!style scope="width:4em;col" | '''Symbol'''

!style scope="width:10em;col" | '''SI units'''

! scope="col" | Intensive (molar)<br />property

! scope="col" | Symbol

! scope="col" | SI units

|-

| style="text-align: left;" | [[Volume (thermodynamics)|Volume]]

| <center>'''V'''</center>

|<center>[[Cubic meter|m³]] <small>or</small> [[Liter|L]]* </center>

| style="text-align: left;" | [[Specific volume]] a.k.a. the [[Multiplicative inverse|reciprocal]] of [[density]]

| [[Specific volume]]***

| <center>'''v'''</center>

|<center>m³/[[Kilogram|kg]] <small>or</small> L*/kg</center>

| style="text-align: left;" | [[Molar volume]]

| ''V''_m

|m³/[[Mole (unit)|mol]] <small>or</small> L/mol

|-

| style="text-align: left;" | [[Internal energy]]

| <center>'''U'''</center>

|<center>[[joule|J]]</center>

| style="text-align: left;" | [[Specific internal energy]]

| <center>'''u'''</center>

|<center>J/kg</center>

| style="text-align: left;" | Molar internal energy

| ''U''_m

|J/mol

|-

| style="text-align: left;" | [[Enthalpy]]

| [[Entropy]]

| <center>''H'S'''</center>

|J

|<center>J/[[Kelvin|K]]</center>

| style="text-align: left;" | [[Specific entropyenthalpy]]

| <center>''h's'''</center>

|J/kg

|<center>J/(kg·K)</center>

| style="text-align: left;" | [[Molar enthalpy]]

| ''H''_m

|J/mol

|-

| style="text-align: left;" | [[Gibbs free energy]]

| [[Enthalpy]]

| <center>''G'H'''</center>

|J

|<center>J</center>

| style="text-align: left;" | Specific Gibbs free energy

| [[Specific enthalpy]]

| <center>''g'h'''</center>

|<center>J/kg</center>

| style="text-align: left;" | [[Chemical potential]]

| ''G''_m <small>or</small> ''μ''

|J/mol

|-

| style="text-align: left;" | [[Entropy]]

| [[Gibbs free energy]]

| <center>''S'G'''</center>

|J/[[Kelvin|K]]

|<center>J</center>

| style="text-align: left;" | [[Specific Gibbs free energyentropy]]

| <center>''s'g'''</center>

|<center>J/(kg</center>·K)

| style="text-align: left;" | [[Molar entropy]]

| ''S''_m

|J/(mol·K)

|-

| style="text-align: left;" | [[Heat capacity]] <br />at constant volume

| <center>'''C_V'''</center>

|J/K

|<center>J/K</center>

| style="text-align: left;" | [[Specific heat capacity]] <br />at constant volume

| <center>'''c_vV'''</center>

|<center>J/(kg·K)</center>

| style="text-align: left;" | [[Molar heat capacity]] <br />at constant volume

| ''C''_''V'',m

|J/(mol·K)

|-

| style="text-align: left;" | [[Heat capacity]] <br />at constant pressure

| <center>'''C_P'''</center>

| J/K

|<center>J/K</center>

| style="text-align: left;" | [[Specific heat capacity]] <br />at constant pressure

| <center>'''c_P'''</center>

|<center> J/(kg·K)</center>

| style="text-align: left;" | [[Molar heat capacity]] <br />at constant pressure

| ''C''_''P'',m

|J/(mol·K)

|}

: * L = [[liter]], J = [[joule]]

: ** specific properties, expressed on a per mass basis

: *** Specific volume is the [[Multiplicative inverse|reciprocal]] of [[density]].

===Molar properties===

If a molecular weight can be assigned for the substance, or the amount of substance (in [[Mole (chemistry)|moles]]) can be determined, then each of these thermodynamic properties may be expressed on a molar basis, and their name may be qualified with the adjective ''molar'', yielding terms such as molar volume, molar internal energy, molar enthalpy, molar entropy. Standards for the symbols of molar quantities do not exist. A well known molar volume is that of an [[ideal gas]] at [[standard conditions for temperature and pressure]], with the value {{gaps|22.41|[[liter]]s/mol}}. Molar Gibbs free energy is commonly referred to as [[chemical potential]], symbolized by μ, particularly when discussing a partial molar Gibbs free energy μ_i for a component i in a mixture.

{{main|Molar quantity}}

If the amount of substance in [[Mole (chemistry)|moles]] can be determined, then each of these thermodynamic properties may be expressed on a molar basis, and their name may be qualified with the adjective '' molar'', yielding terms such as molar volume, molar internal energy, molar enthalpy, and molar entropy. The symbol for molar quantities may be indicated by adding a subscript "m" to the corresponding extensive property. For example, molar enthalpy is <math>H_{\mathrm m}</math>.<ref name="IUPACgreen" /> Molar Gibbs free energy is commonly referred to as [[chemical potential]], symbolized by <math>\mu</math>, particularly when discussing a partial molar Gibbs free energy <math>\mu_i</math> for a component <math>i</math> in a mixture.

==Generality of classification==

For the characterization of substances or reactions, tables usually report the molar properties referred to a [[standard state]]. In that case a superscript <math>^{\circ}</math> is added to the symbol. Examples:

The general validity of the division of physical properties into extensive and intensive kinds has been addressed in the course of science.<ref name=Hatsopoulos>Hatsopoulos G.N. and Keenan J.H. ''Principles of general thermodynamics'', John Wiley and Sons 1965 p.19-20</ref> [[Otto Redlich|Redlich]] noted that physical properties and especially thermodynamic properties are most conveniently defined as either intensive or extensive,<ref name=Redlich>O. Redlich, Journal of chemical education, 47, 154-156 (1970)</ref> however, these two categories are not all-inclusive and some well-defined physical properties conform to neither definition. Redlich also provides examples of mathematical functions that alter the strict additivity relationship for extensive system, such as the square or square root of volume, which occur in some contexts, altbeit rarely used.<ref name=Redlich/>

* <math>V_{\mathrm m}^{\circ}</math> = {{gaps|22.4|[[liter|L]]/mol}} is the molar volume of an [[ideal gas]] at [[standard conditions for temperature and pressure|standard conditions]] of {{gaps|1|[[Standard_atmosphere_(unit)|atm]]}} ({{gaps|101.325|[[Pascal_(unit)|kPa]]}}) and {{gaps|0|[[Celsius|°C]]}} ({{gaps|273.15|[[kelvin|K]]}}).<ref>{{cite book |last1=Petrucci |first1=Ralph H. |last2=Harwood |first2=William S. |last3=Herring |first3=F. Geoffrey |title=General Chemistry |date=2002 |publisher=Prentice Hall |isbn=0-13-014329-4 |page=186 |edition=8th}}</ref>

* <math>C_{P,\mathrm m}^{\circ}</math> is the standard molar heat capacity of a substance at constant pressure.

* <math>\mathrm \Delta_{\mathrm r} H_{\mathrm m}^{\circ}</math> is the standard enthalpy variation of a reaction (with subcases: formation enthalpy, combustion enthalpy...).

* <math>E^{\circ}</math> is the [[standard reduction potential]] of a [[redox couple]], i.e. Gibbs energy over charge, which is measured in [[volt]] = J/C.

==Limitations==

Other systems, for which the standard definitions do not provide a simple answer, are systems in which the subsystems interact when combined. Redlich pointed out that the assignment of some properties as intensive or extensive may depend on the way in which subsystems are arranged. For example, if two identical [[galvanic cell]]s are connected in [[Series and parallel circuits|parallel]], the [[voltage]] of the system is equal to the voltage of each cell, while the [[electric charge]] transferred (or the [[electric current]]) is extensive. However if the same cells are connected in [[Series and parallel circuits|series]], the charge becomes intensive and the voltage extensive.<ref name=Redlich/> The IUPAC definitions do not consider such cases.<ref name=IUPAC/>

The general validity of the division of physical properties into extensive and intensive kinds has been addressed in the course of science.<ref name= "Hatsopoulos">{{cite book | title=Principles of General Thermodynamics | publisher=John Wiley and Sons | author=George N. Hatsopoulos, G. N. | author2=Keenan, J. H. | year=1965 | pages=19–20 | isbn=9780471359999}}</ref> [[Otto Redlich|Redlich]] noted that, although physical properties and especially thermodynamic properties are most conveniently defined as either intensive or extensive, these two categories are not all-inclusive and some well-defined concepts like the square-root of a volume conform to neither definition.<ref name="Redlich">{{cite journal | title=Intensive and Extensive Properties | author=Redlich, O. | journal=J. Chem. Educ. | year=1970 | volume=47 | issue=2 | pages=154–156 | doi=10.1021/ed047p154.2|bibcode = 1970JChEd..47..154R | url=https://escholarship.org/content/qt5mp6r34r/qt5mp6r34r.pdf?t=p0fu3t }}</ref>

Other systems, for which standard definitions do not provide a simple answer, are systems in which the subsystems interact when combined. Redlich pointed out that the assignment of some properties as intensive or extensive may depend on the way subsystems are arranged. For example, if two identical [[galvanic cell]]s are connected in [[Series and parallel circuits|parallel]], the [[voltage]] of the system is equal to the voltage of each cell, while the [[electric charge]] transferred (or the [[electric current]]) is extensive. However, if the same cells are connected in [[Series and parallel circuits|series]], the charge becomes intensive and the voltage extensive.<ref name=Redlich/> The IUPAC definitions do not consider such cases.<ref name=IUPACgreen/>

Some intensive properties do not apply at very small sizes. For example, [[viscosity]] is a [[macroscopic]] [[quantity]] and is not relevant for extremely small systems. Likewise, at a very small scale [[color]] is not independent of size, as shown by [[quantum dots]], whose color depends on the size of the "dot".

==References==

*{{cite book

| first = Herbert B. | last = Callen | authorlink = Herbert Callen | year = 1985

| title = Thermodynamics and an Introduction to Themostatistics | edition = 2nd Ed.

| publisher = John Wiley & Sons | ___location = New York | isbn = 0-471-86256-8 }}

*{{cite book |last=Lewis |first=G.N. |authorlink=Gilbert N. Lewis

|author2=Randall, M. |authorlink2=Merle Randall

|title=Thermodynamics |year=1961 |publisher=McGraw-Hill Book Company

|___location=New York |id= |edition=2nd Edition}}

*{{cite book |last=Linder |first=Bruno. |authorlink=Bruno Linders

|title=Thermodynamics and Introductory Statistical Mechanics |year=2004 |publisher=John Wiley & Sons

|___location=New York |isbn= 0-471-47459-2 }}

{{Reflist}}

==Further reading==

{{cite web |last1=Suresh |title=What is the difference between intensive and extensive properties in thermodynamics? |url=https://callinterview.com/questions-answers/what-is-the-difference-between-intensive-and-extensive-properties-in-thermodynamics/ |website=Callinterview.com |access-date=7 April 2024}}

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