EZsays validly-
There are no boundary conditions defined
Below are some of my notes on how to reach this boundary IN PLANTS. It would if working remand kinds even with mutiple origins of life in the galaxy. If the specifics were prooved then implications for the starting conditions in human monophyly would be apparent.
Dr. Gladyshev @
http://www.endeav.org/evolut/has well writ,
"
Probably, the lack of our knowledge on actual complex systems may be partly attributed to the changes in entropy during this transition, because the entropy cannot be measured directly."
I have not been able to think this outside the green stuff so far.
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As the static dielectric constant can sign a systematic entropic thickness independently of temperature provided an equilibrium is entrained in some attractor of its causal environs the free energy of such a biological dielectric if so polarizable as is a quasi-equilibrium transition temporally coincident/(congruently) with the equilibrium biometrically is in truth actual. If biology correlates a temperature dependence in this volume of material constituents, it may be that the dielectric moment contributes to the thermostat parameters no matter how the macrothermodynamics of capacitive self-energy is measured. It is probable however that physical teleology remands a logic of differences in electrotonic sources and sinks in the variance once quantum mechanical lexicology is invested in the collections responsible for the phenomena.
It is important to notice GG’s We may only discuss the accuracy of the Gibbs thermodynamics as applied to, e.g., quasi-closed systems the processes in which are close to equilibrium. In accord with the very essence of full differential (its mathematical meaning), as well as the first law of thermodynamics, the change in the function of state of the system accompanying the transition from one equilibrium state to another is independent of the way or mechanisms of this transition. Probably, the lack of our knowledge on actual complex systems may be partly attributed to the changes in entropy during this transition, because the entropy cannot be measured directly. The changes in phenomenological entropy accompanying transformations in both simple and complex systems may be calculated only if one has studied the corresponding thermal processes.
The temperature independences might be relatable through the principle of substance stability if the thermostat is not thermostatically strongly correlated transitively across levels.
The equilibration would occur through the process of elastic displacement. Frolich, Equation A 3.4 finds its main application in the case of dielectrics in which polarization is connected with elastic displacement of charges (case (i) of &4). The most general displacement of the dielectric material in a sphere may then be developed in terms of is normal vibrations (cf. van Vleck, V3), and it is then found that the polarizablility alpha is a constant independent of temperature if the density of the substance is kept constant. This procedure is of importance because it shows in a very general way that the assumption of elastic displacement leads to a temperature-independent dielectric constant.
What is at stake is the relative formatting influence of the reductionist(aggregation/aggluntination) vs the holist (differentiation/fragmentation) evolution of the world as presented by Salthe pp143in Evolving Hierarchical Systems. As soon as it is known how the thermostat states are related to phenotypes the differences in relative genetypic frequencies can be assoicatied with the smallest prior fragment fragmentable (due to temporal availability of force) no matter what the figure being formatted is and becomes. If the thermostat is only a property of genetic units, no mater how differentiated the physical means of permitting transitivity across levels will be only that much more determinate and less uncertain. In that case gene expression would be required before one could be most certain of the possible transitions between forms both available and those canalized/constrained. The distinction bears on further functions of action at a distance ultimately. Thus one would have available the form and position of the inducteous body and the nature of the interposed medium (niche construction would have to be defined by then) and it is required to find the changeable distribution of electricity in the inductric. All of this had to do with the resistance that a prior aggreagation bears on a future differentitation.
Elastic Displacment 1/4pie(EdD) (if the displacement D is increased by a small amount dD) (Frohlich 3.4)
Free Energy differnences in the horizontal line below work differences in displacements represented in the vertical below without work of expansion. dU = dQ + E/4pie (dD) (dQ is heat influx) (Frohlich 3.5) Free Energy = U-TS (3.3)
Substance stability(OR EQUIVALENT) l-2
Substance stability l-1
I -3 I-2 I-1 Inititating conditions FOCAL level B+1 B+2 B+3 Boundary conditions
Substance stability l+1
Substance stability l+2
--------------numbers above(+/-) refer to levels of organization------------
The equations are from Frohlich's book on Dielectrics, previously cited on EVC.
This message has been edited by Brad McFall, 07-08-2005 10:09 AM
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