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The jump rate of terminal voltage phase angle is always 2.6 °/ms based on different dynamic reactive power compensation coefficient.
Here, λ is the total instantaneous jump rate, given by λ : = 1 τ ∑ k = 1 P ( θ k + l ( k ) f ¯ k , (1.8).
The larger control parameters (K p or K i) of current inner-loop of rotor-side converter, the bigger jump rate of terminal voltage phase angle.
Our calculations are then used to parameterize the jump rate of Re atoms in W as a function of the underlying stress state.
So a big dynamic reactive power compensation coefficient can reduce maximum jump value and steady-state value of terminal voltage phase angle, and the jump rate of terminal voltage phase angle is unaffected.
Figure 10 shows that the jump rate of terminal voltage phase angle is always 2.6°/ms, and the maximum jump value of terminal voltage phase angle is almost 57.1° based on different fault location and different grid strength.
Similar(35)
With these rates, however, the jump rates are high in regions where the activity is high.
The transition jump rates matrix Γ is not precisely known for the equations.
The jump rates can be computed by discretizing the diffusion equation on that unstructured mesh.
The equations under consideration are more general, whose transition jump rates matrix Q is not precisely known.
where a, b > 0 denotes the unknown transition jump rates subject to a ≤ 2, b ≤ 1, respectively.
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