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Temperature Gibbs energy variation

Thermodynamics is used to predict whether reactants have a spontaneous tendency to change into products. This tendency is associated with a decrease in the free energy or Gibbs energy of the system (G) to a minimum. As a consequence, the thermodynamic criterion for spontaneous change at constant temperature and pressure is AG < 0. Under standard conditions (concentrations = 1 M, and P = 1 atm), the standard Gibbs energy variation (AG°) is related with the equilibrium constant (A) by equation 11 ... [Pg.93]

The enthalpy of fomiation is obtained from enthalpies of combustion, usually made at 298.15 K while the standard entropy at 298.15 K is derived by integration of the heat capacity as a function of temperature from T = 0 K to 298.15 K according to equation (B 1.27.16). The Gibbs-FIehiiholtz relation gives the variation of the Gibbs energy with temperature... [Pg.1904]

The transfer coefficient a has a dual role (1) It determines the dependence of the current on the electrode potential. (2) It gives the variation of the Gibbs energy of activation with potential, and hence affects the temperature dependence of the current. If an experimental value for a is obtained from current-potential curves, its value should be independent of temperature. A small temperature dependence may arise from quantum effects (not treated here), but a strong dependence is not compatible with an outer-sphere mechanism. [Pg.62]

Figure 2.1 The temperature variation of the heat capacity, enthalpy, entropy, and Gibbs energy close to the first-order semiconductor to metal transition in NiS [1]. Figure 2.1 The temperature variation of the heat capacity, enthalpy, entropy, and Gibbs energy close to the first-order semiconductor to metal transition in NiS [1].
Figure 2.3 The temperature variation of the Gibbs energy [5], unit-cell volume [4] enthalpy and heat capacity [5] at the second-order a- to /3-quartz transition of SiC>2-Second-order derivatives of the Gibbs energy like the heat capacity have discontinuities at the transition temperature. Figure 2.3 The temperature variation of the Gibbs energy [5], unit-cell volume [4] enthalpy and heat capacity [5] at the second-order a- to /3-quartz transition of SiC>2-Second-order derivatives of the Gibbs energy like the heat capacity have discontinuities at the transition temperature.
The difference in the Gibbs energies of formation corresponds to the integral of the cell voltage as a function of the composition between the limits of the starting and the final compositions. The value for ASf° is determined from the variation of the cell voltage as a function of the temperature... [Pg.217]

Figure 7.9. Variation of (a) the Gibbs energy, (b) ttie enthalpy and (c) the entropy with temperature (scaled to the nearest-nei bour interaction energy J ) for the complex structure A15. Comparison between BWG CVM in the tetrahedron approximation ( ) and the Monte Carlo method (—) (Turchi and Finel 1992). Figure 7.9. Variation of (a) the Gibbs energy, (b) ttie enthalpy and (c) the entropy with temperature (scaled to the nearest-nei bour interaction energy J ) for the complex structure A15. Comparison between BWG CVM in the tetrahedron approximation ( ) and the Monte Carlo method (—) (Turchi and Finel 1992).
This equilibrium was first studied by Cope et a .54 in 1952. The Gibbs energy difference is small and the rate of interconversion slow at room temperature. Huisgen et al.55 examined the influence of variations of the ethane fragment on the position of the equilibrium. Attachment of a tricarbonyliron moiety apparently causes stabilization of the bicyclo[4.2.0]octadiene system,56 whereas with tricarbonylmolybdenum the monocyclic isomer is isolated as its metal complex.57... [Pg.240]

The allowed variations are then the volume and mole numbers at constant temperature for the Helmholtz energy, and only the mole numbers at constant temperature and pressure for the Gibbs energy. [Pg.98]

Knowledge of these changes in standard Gibbs energy and enthalpy allows one to calculate the equilibrium composition and its variation with temperature. [Pg.18]

Variation of Gibbs Energy, G with Temperature, T at Constant Pressure (dP = 0)... [Pg.57]

Variation of Gibbs Energy, G With Pressure, P at Constant Temperature (dT = 0) and Variation of Entropy, S With Pressure, P at Constant Temperature (dT = 0) for an Idea Gas... [Pg.60]

Variation of Gibbs Energy Function, G Versus Temperature, T for Solid, Liquid and Gaseous Phases... [Pg.64]

The enthalpy function, H, was first introduced in Frame 10, equation (10.8). In Figure 18.1, Frame 18 was shown the general variation of the Gibbs energy G as a function of temperature, T and using the equation ... [Pg.66]


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See also in sourсe #XX -- [ Pg.117 , Pg.118 , Pg.119 ]




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Energy temperatures

Gibbs energy variation with temperature

Gibbs free energy variation with temperature

Standard Gibbs energy change variation with temperature

Temperature variations

The variation of Gibbs energy with temperature

Variation energy

Variational energy

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