Cell Language Theory, The: Connecting Mind And Matter

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338 The Cell Language Theory: Connecting Mind and Matter

b2861 The Cell Language Theory: Connecting Mind and Matter “6x9”

shown in Figure 8.3(d) was successfully simulated using the PDE,
Eq. (8.3), as evident in Figure 8.3(e). It is interesting to note that a double
exponential function, Eq. (8.7), used in [124], can also simulate the same
histogram, with more or less equal effectiveness, although PDE seems to
perform slightly better as indicated by its smaller root mean square devia-
tion (RMSD) value, i.e., 14.80 vs. 15.53 (see Figures 8.3(e) and (f).

y = A(e–Bx – e–Cx), (8.7)

where A, B, and C are free parameters.

8.2.2 Explanation: Quantization of Energy Levels in Enzymes
Just as the fitting of the blackbody radiation spectra to PRE (Planckian
Distribution Equation) is synonymous with the quantization of the energy
levels of electrons in an atom, so it may be concluded that the fitting of
the single-molecule enzyme turnover times to PDE (as demonstrated in
Figure 8.3(e)) may imply the discretization of the conformational states
of an enzyme molecule, in agreement with the concept of “conforma-
tional substrates” of Frauenfelder et al. [125, 126] and the quantization
of the Gibbs free energy levels of an enzyme. This idea is schematically
represented in Figure 8.4.
Blackbody radiation involves promoting the energy levels (vibra-
tional, electronic, or vibronic) of oscillators from their ground state, E 0 , to
higher energy levels, E 1 through E 6. The wavelength of the radiation (or
quantum) absorbed or emitted is given by DE = Ei - E 0 = hu, where Ei is
the ith excited-state energy level, h is the Planck constant, u is the fre-
quency, and DE is the energy absorbed when an oscillator is excited from
its ground state to the ith energy level. Blackbody radiation results when
electrons transition from one energy level to a lower energy level within
matter, e.g., from E 1 to E 0 , from E 2 to E 0 , etc.
A single molecule of cholesterol oxidase is postulated to exist in n
distinct conformational states (i.e., conformational substrates of
Frauenfelder et al. [125]), denoted as Ci with i running from 1 to n. Each
conformational state (or conformer) is thought to exist in a unique Gibbs
free energy level, carries a set of sequence-specific conformational strains
(or conformons) [25, Chapters 8 and 11], and can be excited to a common

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