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Energy Clausius

Equation (A2.1.21) includes, as a special case, the statement dS > 0 for adiabatic processes (for which Dq = 0) and, a fortiori, the same statement about processes that may occur in an isolated system (Dq = T)w = 0). If the universe is an isolated system (an assumption that, however plausible, is not yet subject to experimental verification), the first and second laws lead to the famous statement of Clausius The energy of the universe is constant the entropy of the universe tends always toward a maximum. ... [Pg.341]

See also Ampere, Andre-Marie Clausius, Rudolf Julius Emmanuel Electricity Electricity, History of Faraday, Michael Gibbs, Josiah Willard Magnetism and Magnets Molecular Energy Oersted, Hans Christian Thomson, William. [Pg.783]

This leads to what is called the Clausius form of the second law of thermodynamics. No processes are possible whose only result is the removal of energy from one reservoir and its absorption by another reservoir at a higher temperature. On the other hand, if energy flows from the hot reservoir to the cold reservoir with no other changes in the universe, then the same arguments can be used to show that the entropy increases, nr remains constant for reversible processes. Therefore, such energy flows, which arc vciy familiar, are in agreement with the laws of thermodynamics. [Pg.1130]

Clausius-Clapeyron Equation. This equation was originally derived to describe the vaporization process of a pure liquid, but it can be also applied to other two-phase transitions of a pure substance. The Clausius-Clapeyron equation relates the variation of vapor pressure (P ) with absolute temperature (T) to the molar latent heat of vaporization, i.e., the thermal energy required to vajxirize one mole of the pure liquid ... [Pg.346]

Clausius had shown in 1857 that if K is the translational energy of molecules of a gas and H is the total kinetic energy, then... [Pg.81]

This very important theorem was recognised by R. Clausius in 1850, although he did not at the time give the very simple interpretation, in terms of the conception of intrinsic energy, which was brought forward by Lord Kelvin a year later. [Pg.36]

The entropy and intrinsic energy of steam (or other vapours) may be determined by the following method, due to Clausius. [Pg.184]

Amplitude of a process, 114. Andrew s diagram, 173 Anisotropic bodies, 193 Aphorism of Clausius, 83, 92 Arrhenius theory of electrolytic dissociation, 301 Aschistic process, 31, 36, 51 Atmosphere, 39 Atomic energy, 26 Availability, 65, 66 Available energy, 66, 77, 80, 98, 101... [Pg.539]

Ice type, 195 Ideal gas, 47, 135 Independent variables, 103 Indicator diagram, 45, 127 Inequality of Clausius, 79 Intensity factors, 111 Intrinsic energy, 32, 76, 484 Inversion point, 167 Irreversible processes, 67, 69, 75, 82, 84, 87... [Pg.541]

But just what are the thermodynamic variables that we use to describe a system And what is a system What are Energie (energy) and Entropie (entropy) as described by Clausius We will soon describe the thermodynamic variables of interest. But first we need to be conversant in the language of thermodynamics. [Pg.2]

We earlier referred to an 1865 statement of the First Law given by Clausius, Die Energie der Welt ist Konst ant. [Pg.37]

This simple theory is unsatisfactory, in that the rate of change of the difference in free energy of liquid and crystalline lead predicted by the Clausius-Clapeyron equation leads to a temperature scale for Fig. 8 four... [Pg.595]

It is possible, however, to simplify the calculation of the energy transfer by assuming that the vapor phase is always a saturated vapor. O Connor (Ol) has shown that the rate of approach of a superheated vapor to saturated conditions is extremely rapid when the superheated vapor is in direct contact with its liquid phase. If the vapor phase is assumed to be saturated, the temperature of the phase can be calculated from an integrated form of the Clausius-Clapeyron equation instead of from the vapor-phase energy-transfer equation. [Pg.47]

There are various expressions of the two laws, the most succinct being that of Rudolf Clausius, who (in 1872) wrote The energy of the world is constant. Its entropy tends to a maximum (some authors translate the original German word Welt as universe ). In the 1930s, the second statement led to the idea of the heat death of the universe and caused much speculation. [Pg.238]

First law of thermodynamics (conservation of energy) Rudolph Clausius... [Pg.7]


See other pages where Energy Clausius is mentioned: [Pg.223]    [Pg.207]    [Pg.141]    [Pg.223]    [Pg.207]    [Pg.141]    [Pg.95]    [Pg.768]    [Pg.238]    [Pg.238]    [Pg.626]    [Pg.783]    [Pg.841]    [Pg.1032]    [Pg.1032]    [Pg.1032]    [Pg.1033]    [Pg.1034]    [Pg.1034]    [Pg.1131]    [Pg.1137]    [Pg.28]    [Pg.81]    [Pg.69]    [Pg.87]    [Pg.93]    [Pg.540]    [Pg.93]    [Pg.661]    [Pg.409]    [Pg.236]    [Pg.238]    [Pg.238]    [Pg.265]    [Pg.9]    [Pg.13]   
See also in sourсe #XX -- [ Pg.90 ]




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