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Ten fundamental quantities (Bridgman)
The ten "fundamental quantities" of thermodynamics, according to the 1914 views of American physicist Percy Bridgman. [3]
In language, a quantity, from the Latin quantus “how much”, refers to the measurement of something, in relation to that which can be expressed numerically. [1]

5 principle quantities | Maxwell
The five “principle quantities” in thermodynamics, according to the 1878 views of Scottish physicist James Maxwell, are the energy U, entropy S, volume V, temperature T, and pressure P of a body. [2] Quantities can be either “intensive”, defined uniquely per point in space, or “extensive”, proportional to the dimension of the system.


10 fundamental quantities | Bridgman
The ten "fundamental quantities" in thermodynamics, according to the 1914 views of American physicist Percy Bridgman, are pressure p, temperature τ, volume v, entropy s, heat Q, work W, internal energy E, total heat H (enthalpy), Gibbs potential Z (Gibbs free energy), and Helmholtz potential ψ (Helmholtz free energy), as shown adjacent.

7 base quantities | SI
In 1960, in aims to unify scientific calculations throughout the world, French scientists developed the International System (SI) of units, using the three basic metric (meter-based) units of mass (kg), length (m), time (s), in addition to the four newer units temperature (K), mole (mol), current (A), and light intensity (cd).
SI unit diagram
SI unit relationship diagram.

Derived quantities
All scientific units can be derived from the seven base SI units. The first five SI units (kg, m, s, K, mol) are fairly simple units, whereas the latter two, i.e. current (A), measured in force per distance, and light (cd), being the measure of photon emission from a typical candle, are somewhat more complicated to understand.

One of the more conceptually difficult units to understand is the unit interrelationship involved in the measurement of the mechanical equivalent of heat (J), which involves two derived SI units, work and heat, and one base SI unit, temperature.

References
1. Quantity (definition) – Merriam-Webster Collegiate Dictionary, 2000.
2. (a) Maxwell, James C. (1878). “Tait’s ‘Thermodynamics’ (I)”, (pgs. 257-59). Nature, Jan. 31.
(b) Maxwell, James C. (1878). “Tait’s ‘Thermodynamics’ (II)”, (pgs. 278-81). Nature, Feb. 07.
3. Bridgman, P.W. (1914). "A Complete Collection of Thermodynamic Formulas" (abstract). Phys. Rev. 3 (4): 273–281.

External links
SI base unit – Wikipedia.

EoHT symbol



Sadi-Carnot
Sadi-Carnot
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Petrologist Quantities & qualities 0 Aug 8 2009, 9:19 PM EDT by Petrologist
Thread started: Aug 8 2009, 9:19 PM EDT  Watch
The following are just opinions. Many theorems are applicable by geologists on the spot, in the field. Books' emphases on quantities in thermodynamics often overlooks these.

To read English literature, one needs a dictionary of the period. Similarly, scientific terms change their meanings with time. 'Body' is commonly replaced by 'system' in classical thermodynamics. Scientific objects and their changes (phenomena) are characterized by quantity and quality.

Quantities are specified by three parts: the operation used to obtain it (such as its mass by balance), a unit (such as formula unit of lead oxide: PbO), and the number of units (a number, often from the real number system for continuous models). These correspond to three properties of a vector: its direction, its unit vector, and its magnitude.

Although some scientists deal only with quantities, many thermodynamic theorems are of greater generality. One may need not know the actual vectors involved: homogeneous vectors, rays, or lines may suffice. This blurs the distinction between quantitative and qualitative, for the orientation of colors in a mineral or rocks on the ground may suffice to determine whether temperature had once been increasing or decreasing with time or position.

Russell, B. 1903. The Principles of Mathematics. Cambridge: Cambridge Univ. Press. 534 p.

Meyerson, E. 1930. Identity & Reality. (Trans. from French) London: G. Allen & Unwin. 495 p.

Bridgman, P. 1927. The Logic of Modern Physics. New York: Macmillan. 228 p.

Barrow, G. 1893. On an intrusion of muscovite-biotite gneiss in the south-east Highlands of Scotland. Geol. Soc. London Quart. Jour. v.49, p. 330-58.

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