As overpotentials, either positive or negative, become larger than about 5 × 10−2 volts (V), the second or the first term of equation (3) becomes negligible, respectively.
If however, the tight contact is dominant γ′ in equation (1) is large the previously neglected term of equation (2) permits a non-zero growth rate even for perfectly matching tube catalyst combinations (x=0), for example, armchair on flat substrate.
The results represent the second term of Equation 1 is small and insensitive to temperature.
Now, considering the second term of equation (3.1) and using Abel's lemma (3.3).
The demography-dependent term of equation (7) sums to CHF 2, whereas the independent terms amount to CHF 93.
If the odd subcarriers of X(k) are set to zero, then the second term of Equation 35 is zero.
(9) The last term of equation (8) was introduced at the end to represent the constraint (|mathbf{m}|=1).
The sum in the third term of equation (1) covers all compartments c' which can communicate with compartment c.
The later term of Equation 2 vanishes because B T is always much larger than B i and B so.
Then we express the middle term of equation (12) as the convex combination of the left and right terms.
For small m, the n/m limit improves (increases) since the second term of Equation 20 now dominates.
