Bulk modulus
The bulk modulus ( or ) of a substance measures the substance's resistance to uniform compression. It is defined as the ratio of the infinitesimal pressure increase to the resulting relative decrease of the volume. Its SI unit is the pascal, and its dimensional form is M^{1}L^{−1}T^{−2}.^{1}
Contents
Definition
The bulk modulus can be formally defined by the equation
where is pressure, is volume, and denotes the derivative of pressure with respect to volume. Equivalently
where ρ is density and dP/dρ denotes the derivative of pressure with respect to density. The inverse of the bulk modulus gives a substance's compressibility.
Other moduli describe the material's response (strain) to other kinds of stress: the shear modulus describes the response to shear, and Young's modulus describes the response to linear stress. For a fluid, only the bulk modulus is meaningful. For an 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.
Thermodynamic relation
Strictly speaking, the bulk modulus is a thermodynamic quantity, and in order to specify a bulk modulus it is necessary to specify how the temperature varies during compression: constanttemperature (isothermal ), constantentropy (isentropic ), and other variations are possible. Such distinctions are especially relevant for gases.
For an ideal gas, the isentropic bulk modulus is given by
and the isothermal bulk modulus is given by
where
 γ is the heat capacity ratio
 p is the pressure.
When the gas is not ideal, these equations give only an approximation of the bulk modulus. In a fluid, the bulk modulus K and the density ρ determine the speed of sound c (pressure waves), according to the NewtonLaplace 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.
Measurement
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.
Selected values
Material  Bulk modulus in GPa  Bulk modulus in psi 

Glass (see also diagram below table)  to 35 55  ×10^{6} 5.8 
Steel  160  ×10^{6} 29 
Diamond (at 4K) ^{2}  443  ×10^{6} 64 
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
Water  ×10^{9} Pa (value increases at higher pressures) 2.2 
Methanol  ×10^{8} Pa (at 20 °C and 1 Atm) 8.23 
Air  ×10^{5} Pa (adiabatic bulk modulus) 1.42 
Air  ×10^{5} Pa (constant temperature bulk modulus) 1.01 
Solid helium  ×10^{7} Pa (approximate) 5 
References
 ^ "Bulk Elastic Properties". hyperphysics. Georgia State University.
 ^ Page 52 of "Introduction to Solid State Physics, 8th edition" by Charles Kittel, 2005, ISBN 047141526X
 ^ Fluegel, Alexander. "Bulk modulus calculation of glasses". glassproperties.com.
Further reading
 De Jong, Maarten; Chen, Wei (2015). "Charting the complete elastic properties of inorganic crystalline compounds". Scientific Data 2. doi:10.1038/sdata.2015.9.

Conversion formulas  

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.  
Notes  
There are two valid solutions. 

Cannot be used when  