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In the physical sciences, an intensive property (also called a bulk property, intensive quantity, or intensive variable), is a physical property of a system that does not depend on the system size or the amount of material in the system: it is scale invariant.

By contrast, an extensive property (also extensive quantity, extensive variable, or extensive parameter) is one that is additive for independent, noninteracting subsystems.^[1] It is directly proportional to the amount of material in the system.

For example, density is an intensive property of a substance because it does not depend on the amount of that substance; mass and volume, which are measures of the amount of the substance, are extensive properties. In general the ratio of two extensive properties (such as mass and volume) that scale in the same way is scale-invariant, and hence an intensive property (such as density).

There are also measured physical properties which are neither intensive nor extensive. See counterexamples below.

Intensive properties[link]

An intensive property is a physical quantity whose value does not depend on the amount of the substance for which it is measured. For example, the temperature of a system in thermal equilibrium is the same as the temperature of any part of it. If the system is divided the temperature of each subsystem is identical. The same applies to the density of a homogeneous system: if the system is divided in half, the mass and the volume change in the identical ratio and the density remains unchanged.

According to the state postulate, for a sufficiently simple 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.

Some intensive properties, such as viscosity, are empirical macroscopic quantities and are not relevant to extremely small systems.

Combined intensive properties[link]

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

If a set of parameters, Failed to parse (Missing texvc executable; please see math/README to configure.): \{a_i\} , are intensive properties and another set, Failed to parse (Missing texvc executable; please see math/README to configure.): \{A_j\} , are extensive properties, then the function Failed to parse (Missing texvc executable; please see math/README to configure.): F(\{a_i\},\{A_j\})

is an intensive property if for all Failed to parse (Missing texvc executable; please see math/README to configure.): \alpha

,

Failed to parse (Missing texvc executable; please see math/README to configure.): F(\{a_i\},\{\alpha A_j\}) = F(\{a_i\},\{A_j\}).\,

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).

Joining systems[link]

This section's factual accuracy is disputed. Please help to ensure that disputed facts are reliably sourced. See the relevant discussion on the talk page.

Let there be a system or piece of substance a of amount m_a and another piece of substance b of amount m_b which can be combined without interaction. [For example, lead and tin combine without interaction, but common salt dissolves in water and the properties of the resulting solution are not a simple combination of the properties of its constituents.] Let V be an intensive variable. The value of variable V corresponding to the first substance is V_a, and the value of V corresponding to the second substance is V_b. If the two pieces a and b are put together, forming a piece of substance "a+b" of amount m_a+b = m_a+m_b, then the value of their intensive variable V is:

Failed to parse (Missing texvc executable; please see math/README to configure.): V = \frac{m_a V_a + m_b V_b}{m_a + m_b},

which is a weighted mean. Further, if V_a = V_b then V_{a + b} = V_a = V_b, i.e. the intensive variable is independent of the amount. Note that this property holds only as long as other variables on which the intensive variable depends stay constant.

In a thermodynamic system composed of two monatomic ideal gases, a and b, if the two gases are mixed, the final temperature T is

Failed to parse (Missing texvc executable; please see math/README to configure.): T = \frac{N_aT_a+N_bT_b}{N_a+N_b},

a weighted mean where Failed to parse (Missing texvc executable; please see math/README to configure.): N_i

is the number of particles in gas i, and Failed to parse (Missing texvc executable; please see math/README to configure.): T_i
is the corresponding temperature.

Note that you have to measure the amounts in the same unit that was used to calculate the intensive property from the extensive property. So when you interpolate density, you have to measure the properties in volume, as density is mass per volume. The formula makes no sense when you measure the properties in mass (kg).

Examples[link]

Examples of intensive properties include:

Extensive properties[link]

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.^[1] 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.

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 (extensive) gives density (intensive).

Combined extensive properties[link]

If a set of parameters Failed to parse (Missing texvc executable; please see math/README to configure.): \{a_i\}

are intensive properties and another set Failed to parse (Missing texvc executable; please see math/README to configure.): \{A_j\}
are extensive properties, then the function Failed to parse (Missing texvc executable; please see math/README to configure.): F(\{a_i\},\{A_j\})
is an extensive property if for all Failed to parse (Missing texvc executable; please see math/README to configure.): \alpha

,

Failed to parse (Missing texvc executable; please see math/README to configure.): F(\{a_i\},\{\alpha A_j\})=\alpha F(\{a_i\},\{A_j\}).\,

Thus, extensive properties are homogeneous functions (of degree 1) with respect to Failed to parse (Missing texvc executable; please see math/README to configure.): \{A_j\} . It follows from Euler's homogeneous function theorem that

Failed to parse (Missing texvc executable; please see math/README to configure.): F(\{a_i\},\{A_i\})=\sum_j A_j \left(\frac{\partial F}{\partial A_j}\right),

where the partial derivative is taken with all parameters constant except Failed to parse (Missing texvc executable; please see math/README to configure.): A_j . The converse is also true - any function which obeys the above relationship will be extensive.^{[citation needed]}

Examples[link]

Examples of extensive properties include^{[citation needed]}:

Related extensive and intensive properties[link]

Thermodynamics
Branches Classical · Statistical · Chemical Equilibrium / Non-equilibrium Thermofluids
Laws Zeroth · First · Second · Third
Systems State: Equation of state Ideal gas · Real gas Phase of matter · Equilibrium Control volume · Instruments Processes: Isobaric · Isochoric · Isothermal Adiabatic · Isentropic · Isenthalpic Quasistatic · Polytropic Free expansion Reversibility · Irreversibility Endoreversibility Cycles: Heat engines · Heat pumps Thermal efficiency
System properties Property diagrams Intensive and extensive properties State functions: Temperature / Entropy (intro.) † Pressure / Volume † Chemical potential / Particle no. † († Conjugate variables) Vapor quality Reduced properties Process functions: Work · Heat
Material properties Specific heat capacity  Failed to parse (Missing texvc executable; please see math/README to configure.): c= Failed to parse (Missing texvc executable; please see math/README to configure.): T Failed to parse (Missing texvc executable; please see math/README to configure.): \partial S Failed to parse (Missing texvc executable; please see math/README to configure.): N Failed to parse (Missing texvc executable; please see math/README to configure.): \partial T Compressibility  Failed to parse (Missing texvc executable; please see math/README to configure.): \beta=- Failed to parse (Missing texvc executable; please see math/README to configure.): 1 Failed to parse (Missing texvc executable; please see math/README to configure.): \partial V Failed to parse (Missing texvc executable; please see math/README to configure.): V Failed to parse (Missing texvc executable; please see math/README to configure.): \partial p Thermal expansion  Failed to parse (Missing texvc executable; please see math/README to configure.): \alpha= Failed to parse (Missing texvc executable; please see math/README to configure.): 1 Failed to parse (Missing texvc executable; please see math/README to configure.): \partial V Failed to parse (Missing texvc executable; please see math/README to configure.): V Failed to parse (Missing texvc executable; please see math/README to configure.): \partial T Property database
Equations Carnot's theorem Clausius theorem Fundamental relation Ideal gas law Maxwell relations Table of thermodynamic equations
Potentials Free energy · Free entropy Internal energy Failed to parse (Missing texvc executable; please see math/README to configure.): U(S,V) Enthalpy Failed to parse (Missing texvc executable; please see math/README to configure.): H(S,p)=U+pV Helmholtz free energy Failed to parse (Missing texvc executable; please see math/README to configure.): A(T,V)=U-TS Gibbs free energy Failed to parse (Missing texvc executable; please see math/README to configure.): G(T,p)=H-TS
History and culture Philosophy: Entropy and time · Entropy and life Brownian ratchet Maxwell's demon Heat death paradox Loschmidt's paradox Synergetics History: General · Heat · Entropy · Gas laws Perpetual motion Theories: Caloric theory · Vis viva Theory of heat Mechanical equivalent of heat Motive power Publications: "An Experimental Enquiry Concerning ... Heat" "On the Equilibrium of Heterogeneous Substances" "Reflections on the Motive Power of Fire" Timelines of: Thermodynamics · Heat engines Art: Maxwell's thermodynamic surface Education: Entropy as energy dispersal
Scientists Daniel Bernoulli Sadi Carnot Benoît Paul Émile Clapeyron Rudolf Clausius Hermann von Helmholtz Constantin Carathéodory Pierre Duhem Josiah Willard Gibbs James Prescott Joule James Clerk Maxwell Julius Robert von Mayer William Rankine John Smeaton Georg Ernst Stahl Benjamin Thompson William Thomson, 1st Baron Kelvin John James Waterston
v t e

Although not true for all physical properties, there are a number of properties which have corresponding extensive and intensive analogs, many of which are thermodynamic properties. Examples of such extensive thermodynamic properties, which are dependent on the size of the thermodynamic system in question, include volume (V), internal energy (U), enthalpy (H), entropy (S), Gibbs free energy (G), Helmholtz free energy (A), and heat capacities (C_v and C_p) (in the sense of thermal mass). Note that the main symbols of these extensive thermodynamic properties shown here are capital letters. Except for volume (V), these extensive properties are dependent on the amount of material (substance) in the thermodynamic system in question.

For homogeneous substances, these extensive thermodynamic properties each have analogous intensive thermodynamic properties, which can be expressed on a per mass basis, and the corresponding intensive property symbols would be the lower case letters of the corresponding extensive property. Examples of intensive thermodynamic properties, which are independent on the size of the thermodynamic system in question and are analogous to the extensive ones mentioned above, include specific volume (v), specific internal energy (u), specific enthalpy (h), specific entropy (s), specific Gibbs free energy (g), specific Helmholtz free energy (a), and specific heat capacities (c_v and c_p, sometimes simply called specific heats). These intensive thermodynamic properties are effectively material properties which are valid at a point in a thermodynamic system or at a point in space at a certain time. These intensive properties are dependent on the conditions at that 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. See the table below. Specific volume is volume per mass, the reciprocal of density which equals mass per volume.

* l = liter, J = joule

** specific properties, expressed on a per mass basis

*** Specific volume is the reciprocal of density.

If a molecular weight can be assigned for the substance, or the number of moles in the system can be determined, then each of these thermodynamic properties can be expressed on a per mole basis. These intensive properties could be named after the analogous extensive properties but with the word "molar" preceding them; thus molar volume, molar internal energy, molar enthalpy, molar entropy, etc. Although the same small letters can be used as in the analogous specific properties indicating they are intensive, sometimes the corresponding capital letters have been used (and understood to be on a per mole basis), and there seems to be no universally agreed upon symbol convention for these molar properties. A well known molar volume is that of an ideal gas at STP (Standard Temperature and Pressure); this molar volume = 22.41 liters per mole. 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.

Counter-examples[link]

There are measured physical properties which are neither intensive nor extensive. For example the electrical resistance of two resistors is the sum of their two resistances only if the resistors are connected in series, but not if they are connected in parallel (if they are placed in parallel, it is instead the electrical conductance, the inverse of the resistance, of the two resistors that is the sum of their two conductances). The electrical resistance of independent noninteracting resistors (subsystems) is therefore not additive in general, and electrical resistance is not an extensive property. Nor is it intensive because the resistance of the two resistors is not equal in general, even if they consist of the same material at the same temperature and pressure.

Another counter-example is invariant mass in special relativity, which is not additive for subsystems in motion relative to each other. Invariant mass is therefore not an extensive quantity, nor it is an intensive quantity.

References[link]

• Callen, Herbert B. (1985). Thermodynamics and an Introduction to Themostatistics (2nd Ed. ed.). New York: John Wiley & Sons. ISBN 0-471-86256-8. 
• Lewis, G.N.; Randall, M. (1961). Thermodynamics (2nd Edition ed.). New York: McGraw-Hill Book Company.