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In order to explain the observed display of wave propagation phenomena such as beam deviation, we use finite element modeling.
The key concept is the combination of polarization/image rotation, the 90° optical beam deviation, and the optical beam alignment via mirror technology.
Though the signal cancellation can be avoided by accurate estimation of the auxiliary steering vector of the desired signal which results in a computational cost of O(K 1 N m N a + K 1 N m ), the gain loss of the desired signal resulted from the main beam deviation still exists.
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The feature of the model is accounting the electron beam (EB) deviation from the ideal position based on manipulators errors.
Such a system uses the received signal to estimate the beam pointing deviation and then adjusts the antenna pointing.
Simulating incoming beams of different angles (α ∈ [45°, 90°]) reveals a shift of the spot centroid of up to 1.8 mm, a change of the reflection profile scale of approximately 250% and an increase of the beam standard deviation of up to 5 mm.
Two optimization models are developed and simulated by Xian Liu for continuously adjusting the transmitter power, wavelength, telescope gain to mitigate the beam LoS deviations due to building sway, and atmospheric interference.
The analyses demonstrated that the positioning deviations of 48 beam lines satisfy the deviation budget requirements.
This was necessary in order to avoid plastic deformation of the beams and crack deviation out of the inter-laminar plane.
For delaminations of only 10% of the length of a composite beam, modal frequency deviations of about 20% were observed numerically and experimentally.
The expanded discussion of the stiffness tensor now explains how the anisotropy of a beam leads to deviations from simple, 1-dimensional buckling.
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