The bulk modulus ( or ) of a substance is a measure of the resistance of a substance to compression. It is defined as the ratio of the infinitesimal pressure increase to the resulting relative decrease of the volume.
Other moduli describe the material's response (strain) to other kinds of stress: the shear modulus describes the response to shear stress, and Young's modulus describes the response to normal (lengthwise stretching) stress. For a fluid, only the bulk modulus is meaningful. For a complex anisotropic solid such as wood or paper, these three moduli do not contain enough information to describe its behaviour, and one must use the full generalized Hooke's law. The reciprocal of the bulk modulus at fixed temperature is called the isothermal compressibility.
The bulk modulus (which is usually positive) can be formally defined by the equation
where is pressure, is the initial volume of the substance, and denotes the derivative of pressure with respect to volume. Since the volume is inversely proportional to the density, it follows that
where is the initial density and denotes the derivative of pressure with respect to density. The inverse of the bulk modulus gives a substance's compressibility. Generally the bulk modulus is defined at constant temperature as the isothermal bulk modulus, but can also be defined at constant entropy as the adiabatic bulk modulus.
Strictly speaking, the bulk modulus is a thermodynamic quantity, and in order to specify a bulk modulus it is necessary to specify how the pressure varies during compression: constant-temperature (isothermal ), constant-entropy (isentropic ), and other variations are possible. Such distinctions are especially relevant for gases.
For an ideal gas, an isentropic process has:
where is the heat capacity ratio. Therefore, the isentropic bulk modulus is given by
Similarly, an isothermal process of an ideal gas has:
Therefore, the isothermal bulk modulus is given by
When the gas is not ideal, these equations give only an approximation of the bulk modulus. In a fluid, the bulk modulus and the density determine the speed of sound (pressure waves), according to the Newton-Laplace formula
In solids, and have very similar values. Solids can also sustain transverse waves: for these materials one additional elastic modulus, for example the shear modulus, is needed to determine wave speeds.
It is possible to measure the bulk modulus using powder diffraction under applied pressure. It is a property of a fluid which shows its ability to change its volume under its pressure.
|Material||Bulk modulus in GPa||Bulk modulus in Mpsi|
|Diamond (at 4K) ||443||64|
|Alumina (γ phase)||162 ± 14||23.5|
|Glass (see also diagram below table)||35 to 55||5.8|
|Graphite 2H (single crystal)||34||4.9|
|Rubber||1.5 to 2||0.22 to 0.29|
A material with a bulk modulus of 35 GPa loses one percent of its volume when subjected to an external pressure of 0.35 GPa (~3500 bar) (assumed constant or weakly pressure dependent bulk modulus).
|β-Carbon nitride||427±15 GPa (predicted)|
|Water||2.2 GPa (0.32 Mpsi) (value increases at higher pressures)|
|Methanol||823 MPa (at 20 °C and 1 Atm)|
|Solid helium||50 MPa (approximate)|
|Air||142 kPa (adiabatic bulk modulus [or isentropic bulk modulus])|
|Air||101 kPa (isothermal bulk modulus)|
Interatomic potential and linear elasticity
Since linear elasticity is a direct result of interatomic interaction, it is related to the extension/compression of bonds. It can then be derived from the interatomic potential for crystalline materials. First, let us examine the potential energy of two interacting atoms. Starting from very far points, they will feel an attraction towards each other. As they approach each other, their potential energy will decrease. On the other hand, when two atoms are very close to each other, their total energy will be very high due to repulsive interaction. Together, these potentials guarantee an interatomic distance that achieves a minimal energy state. This occurs at some distance a0, where the total force is zero:
Where U is interatomic potential and r is the interatomic distance. This means the atoms are in equilibrium.
To extend the two atoms approach into solid, consider a simple model, say, a 1-D array of one element with interatomic distance of a, and the equilibrium distance is a0. Its potential energy-interatomic distance relationship has similar form as the two atoms case, which reaches minimal at a0, The Taylor expansion for this is:
At equilibrium, the first derivative is 0, so the dominate term is the quadratic one. When displacement is small, the higher order terms should be omitted. The expression becomes:
Which is clearly linear elasticity.
Note that the derivation is done considering two neighboring atoms, so the Hook's coefficient is:
This form can be easily extended to 3-D case, with volume per atom(Ω) in place of interatomic distance.
Relationship with atomic radius
As derived above, the bulk modulus is directly related the interatomic potential and volume per atoms. We can further evaluate the interatomic potential to connect K with other properties. Usually, the interatomic potential can be expressed as a function of distance that has two terms, one term for attraction and another term for repulsion.
Where A > 0 represents the attraction term and B > 0 represents repulsion. n and m are usually integral, and m is usually larger than n, which represents short range nature of repulsion. At equilibrium position, u is at its minimal, so first order derivative is 0.
when r is close to, recall that the n (usually 1 to 6) is smaller than m (usually 9 to 12), ignore the second term, evaluate the second derivative
Recall the relationship between r and Ω
In many cases, such as in metal or ionic material, the attraction force is electrostatic, so n = 1, we have
This applies to atoms with similar bonding nature. This relationship is verified within alkali metals and many ionic compounds.
- ^ "Bulk Elastic Properties". hyperphysics. Georgia State University.
- ^ Page 52 of "Introduction to Solid State Physics, 8th edition" by Charles Kittel, 2005, ISBN 0-471-41526-X
- ^ Gallas, Marcia R.; Piermarini, Gasper J. (1994). "Bulk Modulus and Young's Modulus of Nanocrystalline γ-Alumina". Journal of the American Ceramic Society. 77 (11): 2917–2920. doi:10.1111/j.1151-2916.1994.tb04524.x. ISSN 1551-2916.
- ^ "Graphite Properties Page by John A. Jaszczak". pages.mtu.edu. Retrieved 2021-07-16.
- ^ "Silicone Rubber". AZO materials.
- ^ Fluegel, Alexander. "Bulk modulus calculation of glasses". glassproperties.com.
- ^ Liu, A. Y.; Cohen, M. L. (1989). "Prediction of New Low Compressibility Solids". Science. 245 (4920): 841–842.
- ^ H., Courtney, Thomas (2013). Mechanical Behavior of Materials (2nd ed. Reimp ed.). New Delhi: McGraw Hill Education (India). ISBN 978-1259027512. OCLC 929663641.
- ^ Gilman, J.J. (1969). Micromechanics of Flow in Solids. New York: McGraw-Hill. p. 29.
- De Jong, Maarten; Chen, Wei (2015). "Charting the complete elastic properties of inorganic crystalline compounds". Scientific Data. 2: 150009. Bibcode:2013NatSD...2E0009D. doi:10.1038/sdata.2015.9. PMC 4432655. PMID 25984348.
|Homogeneous isotropic linear elastic materials have their elastic properties uniquely determined by any two moduli among these; thus, given any two, any other of the elastic moduli can be calculated according to these formulas, provided both for 3D materials (first part of the table) and for 2D materials (second part).|
There are two valid solutions.
|Cannot be used when|
|Cannot be used when|