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The gray opened circles are the normalized current I k from an individual simulation run.
The multiple access interference (MAI) I k from user k that transmits data with rate can be written as (8).
Together with inequality (1.22), we can get W i ( K ) ≥ W i ( Γ p, i Γ − p, i K ) ≥ W ˜ i ( Γ − p, i K ), from this, we can get inequality (1.23).
The ith microphone signal y i (k) can be expressed as the convolution of the speech signal s(k) with the acoustic impulse response h i (k) from the speech source to the ith microphone plus an additive noise term n i (k).
If, at some time,cell i jumps down and cell k jumps up, then we will define a map Π i k from the ( s j, s k ) phase plane to the ( s i, s j ) phase plane that gives the position of ( s i, s j ) when cell k jumps down.
For each, i = 1, …, I, Node i can obtain ϕ i from an initialization stage in which it receives υ i, k, from each Node k, with k ∈ I i.
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20 Yes Soma I K quote from the review in Llinas and Walton 1990).
The total interference I k emanating from r i n g k is bounded by begin{aligned} I_{k}&={sumnolimits}_{w in text{ring}^{k}} Pd w,v)^{-alpha} &leq {8 2k+1) P((rho-1 k rho-1 kpha}} end{aligned} (5).
The indices i (k) range from 1 to N i (N k ), and in the following we have used N i = N k = N.
Our calculations show that the slope of the curve in I K increased from 1.36 (day 23), to 1.64 (day 30), and finally to 2.34 (day 37).
On substituting the values of φ1, ψ i and δ i (1 ≤ i ≤ k) from Equations 38 to 40 into Equation 24 and after doing some algebraic manipulations, we obtain δ k + 1 = L N − ρ 1 + L N − ρ Open image in new window (41).
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