The length (or distance of propagation along the longitudinal axis) and speed of contractions was measured (Table S5 and Table S6).
In addition, as the influence of prior knowledge would decrease with the propagation distance, the length of the propagation routine becomes more and more limited.
We denote by LTU = 2 and LHT = 3 the maximum impulse response length of the propagation channels in TU50 and HT200 environments, respectively (Figures 10 and 11).
This effect is presumably due to a lowering of thermal conductivity of the BCP film by nanoparticles that scatter the phonons thereby decreasing the mean free path length of phonon propagation.
The factors that would seriously affect this issue are pumping rate of the acid, sufficient length of acidizing propagation, the contact time between acid and rock, closure stress and fluid loss of the acid, etc, and these significant parameters are shown in Fig. 1 specifically.
Fast fading is especially troublesome at frequencies above one gigahertz, where even a few centimetres of difference in the lengths of the propagation paths can significantly change the relative phases of the multipath signals.
Foot-to-foot PWV (PWVff) were computed as Δ L/Δ t, with Δ L the distance traveled by the pulse wave, calculated as the difference between lengths of wave propagation from the heart (4) Δ L = ‖ L heart-artery 1 − L heart-artery2 ‖ and Δ t the transit time between the feet of the pressure waveforms.
In [17], time is divided into slots with length of the maximal propagation delay.
The curves of propagation length are nearly parabolic, and the propagation length increases with the increase of Ht.
The presence of the substrate breaks the symmetry of SP mode, leading to the dramatic decrease of propagation length.
