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To people with the condition the world can appear chaotic with no clear boundaries, order or meaning.
The results revealed that domain boundaries (order variant) and lamellar interfaces (order variant, true twin and pseudo-twin) are relatively transparent to dislocation propagation, but they present significant differences in the geometrical alignment between the incoming and outgoing slip systems.
Therefore the boundary between the two counties was realigned in favour of Worcestershire, as a consequence of the Warwickshire and Worcestershire (Boundaries) Order 1969 legislation (Fig 7).
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Thus, the boundary order-1 limit cycle ((x^{T}(t), 0)) is globally attractive.
Figure 8 Stability of boundary order-1 limit cycle (pmb{(x^{T}(t),0)}).
The boundary order-1 limit cycle ((x^{T}(t), 0)) is unstable for (SC11) and (SC2).
In conclusion, we have the following main results for the boundary order-1 limit cycle.
Thus, the boundary order-1 limit cycle is globally stable if (tau=0) and (A_{h}neq0) in case (SC123).
As (A_{h}) increases and goes beyond zero (i.e. (A_{h}>0)), then the boundary order-1 limit cycles disappear.
The boundary order-1 limit cycle ((x^{T}(t), 0)) is globally asymptotically stable for (SC123), and it is locally asymptotically stable for (SC12).
The local stability of the boundary order-1 limit cycle for (SC12) is obvious due to the domain of the phase set.
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Since I tried Ludwig back in 2017, I have been constantly using it in both editing and translation. Ever since, I suggest it to my translators at ProSciEditing.

Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com