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In this section, we will analyze the oscillation mode in detail.
In the following, we will investigate the oscillation mode in detail, assuming that we are trying to explain the PP oscillation in terms of the two-room model.
Next, we discuss how to compute D(X i, Y k ) for all permutations { Y1, Y2,…, Y K } in a batch mode in detail.
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It is shown that the directional frequency response functions are useful in identifying the strength of modes in detail, or equivalently, the modes of symmetry, anisotropy, asymmetry and coupled asymmetry.
We will present the contributions from higher modes in detail in our future work.
It involves the free energy decomposition involving MM-PBSA method [ 2, 3, 7– 11] and MM-GBSA method [ 3, 12] to investigate the binding modes in detail at the atomic level and also to estimate protein stabilities [ 13].
As stated above, our intention was not to describe the flow through the porous scaffold itself, which would require a different approach, but to examine the flow and pressure characteristics of the bioreactor during operational mode in more detail.
Most of the elements shown in Figure 2 will be explained in mode detail in the remainder of this section.
Three wave modes are investigated in detail: fundamental the ion Bernstein mode (IB1), second harmonic of ion Bernstein mode (IB2), and oblique ion cyclotron mode (IC).
Fundamental TMz101 mode is explored in detail.
The influence of spatial variations of the bulk properties on the propagating mode is described in detail.
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