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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.
Now, considering the first term of equation (3.1), (3.2).
The first term of Equation 3 corresponds to the direct-path signal captured by the microphone and is represented by the solid line in Figure3.
The first term of Equation 6 considers only the current frame Y t), while the succeeding terms consider the left context.
end{aligned} (16) Let us check the first term of equation (16), which has an indetermination at (tau=t), then we can analyze the corresponding limitation by the L'Hopital rule.
In this assumption, the first term of Equation 6 can be disregarded and the approximations for sinusoidal function in the second term, sin(x) ≈ x and cos(x) ≈ 1, would be valid.
Similar(32)
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).
If the odd subcarriers of X(k) are set to zero, then the second term of Equation 35 is zero.
For small m, the n/m limit improves (increases) since the second term of Equation 20 now dominates.
The sum in the third term of equation (1) covers all compartments c' which can communicate with compartment c.
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