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When compared with literature data, the current results are in fair agreement when only spontaneous and single-reflected re-initiation modes are considered, but when multiple reflections are included, the go/no-go boundary for successful transmission is much wider than found from the limited literature data available.
Multiple reflections are neglected here as their effects rapidly diminish with the reflectance R < 0.005 for all rays.
By modeling the cavities together, coupling effects are enforced directly and multiple reflections are readily observable.
It is furthermore demonstrated that the amplitude of the back-scattered signal received by the transceiver results mainly from a single reflection on particles, whereas echoes experiencing multiple reflections are strongly damped.
The absorption coefficient can be determined from the normal incidence transmission through plane-parallel plate of thickness (d), and interference and multiple reflections are neglected.
The phenomena of partial absorption, transmission, and multiple reflections are repeated in each subsequent layer resulting in more radiation absorption within the bulk of the sample resulting in higher SE due to absorption.
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Multiple reflections also increase SER but the effect of multiple reflections is more prominent on SEA.
Defining M = tmax/Δt and assuming as the time origin the arrival of the LOS component, the impulse response after multiple reflections is given by ∑ k = 1 ∞ h k t ; E, R = ∑ j = 0 M - 1 p k δ t - jΔt. (6).
Otherwise, multiple reflection is needed and the sample point is in NLOS severe state.
Prominent Fabry-Perot interference fringes attributed to multiple-layer-substrate reflections are observed at a long wavelength.
Although the phenomenon of resonant like amplification behaviour of the structure caused by multiple wave reflections is well known, the potentials for such periodic amplification behaviour are not explicitly considered in code models.
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