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The estimated propagation loss of straight rib-waveguides is 0.7 dB/cm at 1.55 μm.
The BTB-TDMA determines transmission schedule of UNs based on UNs' estimated propagation delays (EPDs), reflecting on UNs' mobility.
Finally, numerical results show, in a preliminary way, how the identified source strength converges towards the exact velocity when the estimated propagation model tends to the exact propagation model.
The first column shows the dependence of time to peak of the LFP as a function of the cortical distance from the triggering electrode, and estimated propagation velocities.
The estimated propagation velocities of the post-seismic TEC disturbances during the main shock (0.89 km/s) and aftershock (0.77 km/s) confirm the presence of an acoustic frequency as the generative mode for the observed TEC fluctuations.
As an example, using Weissberger's model for a foliage depth of 10 m the estimated propagation loss of 7.4 dB due to the foliage obstruction at 5.67 GHz is 3.4 dB higher than the loss experiences at 630 MHz.
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Using the timestamp, a node estimates propagation delay to the coordinator (PDC) in order to reduce guard time while transmitting a packet.
We also present an approach to obtain uncertainty bounds on estimated error propagation probability (EPP) values used in our SER modeling framework.
Using shock parameters in the solar wind and observations of the shock in the magnetosheath, we estimated the propagation speed of the corresponding magnetosheath disturbance.
Confidence intervals on crack growth parameters that were estimated from propagation of errors solutions were comparable to those from Monte Carlo simulation.
The accuracy of estimated ISW propagation speeds is also tested by tracking the signals of ISWs using two ADCP moorings and it is found that the prediction deviation is less than 10%.
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