We should notice that with the above parameters, the approximation considered in Eq. (10) is still valid.
Make an approximation, consider the second-order term in.
We begin with the approximation (29).
This approximation conforms with the approximation for UTR length given by Hurowitz et al [ 17].
Remark that, with strong approximation, we consider that random mating do not alter the percentage of the two parts of the populations, thus we consider only the changes due to fit parents producing unfit offspring, and to unfit parents producing fit offspring.
For the approximation of (12), we consider the following theorem.
In general, the model with the lowest AIC is considered the best approximation to the data.
In essence, this paper replaces the microphone-received signal with for TDE since can be considered as the approximation of.
Consequently, for each value of n Rydberg states with ℓ≥4 can, to a good approximation, be considered degenerate in energy in the same way that all states in the H atom, or other hydrogenic atoms (e.g., D, T, He +, Li 2+, (overline {mathrm {H}}) and Ps), are.
Second, we considered the approximation coefficients of all levels, instead of the detail coefficients.
We consider the approximation of Reissner Mindlin plates with curved boundaries, using a p-version MITC finite element method.
