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The modeled delay captured spatial extent of lee wave signals on the east side of the Hidaka Mountains, although the topography-correlated delay was also significant in the modeled delay.
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Analytic expressions for throughput, delay, capture probability, energy, and energy efficiency are derived.
Here, the closed interval should be filtered based on the network delay, delay capture and the complexity of the distribution complex degree.
Then, in Section 4, based on the obtained system state probabilities, expressions for throughput, delay, capture probability, energy, and energy efficiency are developed and two stability conditions are set.
In this context, we characterize the system through an MPR model and a finite Markov chain, and derive accordingly analytic expressions for throughput, delay, capture probability (or reliability), energy, and energy efficiency.
F{P}_i=left{{x}_i D{F}_i+{tau}_{mto n}left({x}_i-{x}_{i-1}right){leftVert ArightVert}^2right} (8) Here, the closed interval should be filtered based on the network delay, delay capture and the complexity of the distribution complex degree.
we characterize analytically the FF-NDMA protocol in terms of throughput, delay, capture probability (i.e., probability of a successful transmission or, equivalently, reliability of the protocol), energy, and energy efficiency (i.e., efficiency of the protocol, which is measured through a throughput-energy ratio).
Therefore, π can be obtained as the normalized single eigenvector associated with the unit eigenvalue of P. In this section, we derive throughput, delay, capture probability, energy, and energy efficiency for FF-NDMA by using the steady-state probabilities obtained in Section 3.2.
In this section, we evaluate the FF-NDMA protocol in terms of throughput, delay, capture probability, energy, and energy efficiency so as to devise the most suitable CP length (R) as a function of the the offered load (G=σK) and the SNR.
In Eq. (11), the variable δ delay(k) captures the delay of the impulse response between the loudspeaker and the belt microphone.
In the case of Hokkaido, the simulated propagation delay well captured amplitude and wavelength of the observed phase variation along a profile shown in Fig. 8.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com