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Creation Energy

In photosynthesis, absorbed solar radiation is captured as chemical energy. In this spontaneous natural conversion of absorbed solar radiation, the solar energy efficiency ranges from 0.8% for land plants to 6.6% for sea plants. In laboratory experiments efficiencies above 30% have been observed. Table 17.1 summarizes the results of solar energy conversion, as discussed in this chapter and where the value for wind energy creation is given as reported in [14]. [Pg.318]

There are two incompatible sayings in present-day thermodynamic usage. These are, firstly, that the entropy is always on the increase (true) and secondly, that energy can neither be created nor destroyed (false, but rather popular). The former asserts that there is a continuous supply of energy, and the latter, based on lWs = lJ, rather than IW s irrev IJ, denies the existence of such an energy supply. Energy creation occurs in Figure 3.1. [Pg.6]

This paper has shown that carbon in the presence of molten salts plays a major role in the extfaction of metals where energy is consumed but, perhaps, more important is that it can make a significant contribution to energy creation and storage under conditions where it is not consumed but simply acts as an intermediate allowing other reactions to take place. In the carbonate fuel cell, the carbonate ion is not consumed but is... [Pg.14]

Figure Al.6.20. (Left) Level scheme and nomenclature used in (a) single time-delay CARS, (b) Two-time delay CARS ((TD) CARS). The wavepacket is excited by cOp, then transferred back to the ground state by with Raman shift oij. Its evolution is then monitored by tOp (after [44])- (Right) Relevant potential energy surfaces for the iodine molecule. The creation of the wavepacket in the excited state is done by oip. The transfer to the final state is shown by the dashed arrows according to the state one wants to populate (after [44]). Figure Al.6.20. (Left) Level scheme and nomenclature used in (a) single time-delay CARS, (b) Two-time delay CARS ((TD) CARS). The wavepacket is excited by cOp, then transferred back to the ground state by with Raman shift oij. Its evolution is then monitored by tOp (after [44])- (Right) Relevant potential energy surfaces for the iodine molecule. The creation of the wavepacket in the excited state is done by oip. The transfer to the final state is shown by the dashed arrows according to the state one wants to populate (after [44]).
Two subsystems a. and p, in each of which the potentials T,p, and all the p-s are unifonn, are pennitted to interact and come to equilibrium. At equilibrium all infinitesimal processes are reversible, so for the overall system (a + P), which may be regarded as isolated, the quantities conserved include not only energy, volume and numbers of moles, but also entropy, i.e. there is no entropy creation in a system at equilibrium. One now... [Pg.343]

Here ak a ) is the annihilation (creation) operator of an exciton with the momentum k and energy Ek, operator an(a ) annihilates (creates) an exciton at the n-th site, 6,(6lt,) is the annihilation (creation) operator of a phonon with the momentum q and energy u) q), x q) is the exciton-phonon coupling function, N is the total number of crystal molecules. The exciton energy is Ek = fo + tfcj where eo is the change of the energy of a crystal molecule with excitation, and tk is the Fourier transform of the energy transfer matrix elements. [Pg.445]

Fig. 3.11 The creation of a band of energy levels from the overlap of two, three, four, etc. atomic orbitals, which eventually gives rise to a continuum. Also shown are the conceptual differences between metals, insulators and semiconductors. Fig. 3.11 The creation of a band of energy levels from the overlap of two, three, four, etc. atomic orbitals, which eventually gives rise to a continuum. Also shown are the conceptual differences between metals, insulators and semiconductors.
The most direct effect of defects on tire properties of a material usually derive from altered ionic conductivity and diffusion properties. So-called superionic conductors materials which have an ionic conductivity comparable to that of molten salts. This h conductivity is due to the presence of defects, which can be introduced thermally or the presence of impurities. Diffusion affects important processes such as corrosion z catalysis. The specific heat capacity is also affected near the melting temperature the h capacity of a defective material is higher than for the equivalent ideal crystal. This refle the fact that the creation of defects is enthalpically unfavourable but is more than comp sated for by the increase in entropy, so leading to an overall decrease in the free energy... [Pg.639]

Electron Capture and /5" "-Decay. These processes are essentially the inverse of the j3 -decay in that the parent atom of Z andM transmutes into one of Z — 1 andM. This mode of decay can occur by the capture of an atomic electron by the nucleus, thereby converting a proton into a neutron. The loss of one lepton (the electron) requires the creation of another lepton (a neutrino) that carries off the excess energy, namely Q — — Z(e ), where the last term is the energy by which the electron was bound to the atom before it was captured. So the process is equivalent to... [Pg.448]

The creation of sugar in the leaves of natural plants is considered the most efficient way of capturing solar energy. Table 1 illustrates the area of land needed to capture 27.7 x 10 kj (6.61 x 10 kcal) of solar energy (2) in various food products. [Pg.40]

In pure and stoichiometric compounds, intrinsic defects are formed for energetic reasons. Intrinsic ionic conduction, or creation of thermal vacancies by Frenkel, ie, vacancy plus interstitial lattice defects, or by Schottky, cation and anion vacancies, mechanisms can be expressed in terms of an equilibrium constant and, therefore, as a free energy for the formation of defects, If the ion is to jump into a normally occupied lattice site, a term for... [Pg.352]


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See also in sourсe #XX -- [ Pg.85 ]




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