theorem of corresponding states

In 1895, Lorentz further elaborated on his theory and introduced the "theorem of corresponding states".

Also Lorentz, by extending his theorem of corresponding states, derived in 1899 the complete transformations.

This is the basis premises of three-parameter theorem of corresponding states:

A fundamental concept of Lorentz's theory in 1895 was the "theorem of corresponding states" for terms of order v/c.

Theorem of corresponding states on SklogWiki.

These dimensionless thermodynamic coordinates, taken together with a substance's compressibility factor, provide the basis for the simplest form of the theorem of corresponding states.

Regarding Lorentz's work before 1905, Brown wrote about the development of Lorentz's "theorem of corresponding states" and then continued:

Whereas Lorentz, in his theorem of corresponding states, had from 1899 effectively assumed this extension of the relativity principle up to second-order effects, Poincaré took it to hold for all orders.

Referring to the critique of Poincaré from 1900, Lorentz wrote in his famous paper in 1904, where he extended his theorem of corresponding states: "Surely, the course of inventing special hypotheses for each new experimental result is somewhat artificial.

An important part of the theorem of corresponding states in 1892 and 1895 was the local time , where t is the time coordinate for an observer resting in the ether, and t is the time coordinate for an observer moving in the ether.

According to van der Waals, the theorem of corresponding states (or principle of corresponding states) indicates that all fluids, when compared at the same reduced temperature and reduced pressure, have approximately the same compressibility factor and all deviate from ideal gas behavior to about the same degree.

Lattice proteins do not have genuine secondary structure; however, some researchers have claimed that they can be extrapolated onto real protein structures which do include secondary structure, by appealing to the same law by which the phase diagrams of different substances can be scaled onto one another (the theorem of corresponding states).