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The results of the 1D and 2D EAST viscous and inviscid simulations using a simplified physical model are presented.
Based on the discussion mentioned above, the similarity coefficients and similarity indices of the physical model are obtained as shown in Tables 5 and 6.
In the meantime, the temperature-rise tests for the critical components and physical model are controlled by BP algorithm which saved experimental periods and improved the conventional efficient.
Operation and cleaning of the physical model are automated in order to enable a single person to give consecutive presentations within a few minutes.
The results shown in Figure 19 demonstrate that our proposed physical parameters outperform the features traditionally used for stress detection, which suggests that parameters estimated from a physical model are more effective at representing stress during phonation than traditional methods.
Ultimately, the means to achieve the end result of a physical model are not relevant to the outcomes of the study, as the primary objective was to test a physical model as opposed to blueprints or a CAD model.
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Therefore, to understand the underlying physics of this nonlinearity in magnetization, a more complete physical model is highly demanded.
Once the design is set, the physical model is digitized by plotting various coordinates, using a tool developed for neurosurgeons.
The physical model is established and solved.
In this paper, a two-dimensional physical model was developed.
The experimental physical model was compared with the Merchant equation.
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