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Exact(5)
where g could be any of ĝ SE , ĝ N G or μ ̂ β , and the sign " + " or "−" must be chosen for the case of a maximum or minimum, respectively; g ′ and g ′′ are the first and second order derivatives, respectively, whose formulae can be derived from Equations (36), (37) or (39), providing similar computation complexity.
The photocurrent J ph for V > V 0 can be derived from Equations 3-5 and 14 as follows: (15).
Hence the cost value, C, of the scheduler can be derived from Equations (12) and (15) as follows: C = FT - T, (16).
Though this phenomenon is not generally recognized in the literature, a special case can actually be derived from equations in Gillespie's 1977 paper [ 27] and in Proulx [ 9].
Equation (2) can be derived from equations (1) following [ 20] (chapt. 13) by assuming the stationary case, i.e., i.e. for { v i | v i ≠ 0}.
Similar(54)
Equation (2), known as the Nernst equation, which can be derived from equation (1), gives the value of the electrode potential when the rate of oxidation exactly equals the rate of reduction.
Its expression can be derived from Equation (20).
From these equalities, Equation (26) can be derived from Equation (28).
This conclusion can directly be derived from Equation (25) or (27).
The estimated total received power PS (coherent signal power) can be derived from Equation 3.
The exciton separation rate k s(E) can be derived from Equation 6-9, (11).
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