We choose an order on (V) by rotative plane sweep.
The criteria to choose an order expansion is the critical Rayleigh number where the bifurcation takes place does not change if we increase further the order expansion.
In practice, a useful heuristic is first to choose an order of the taxa such that a large subset of the given set of splits is circular.
In an active setting, experimental design is used to choose an order of perturbations (from a set of feasible candidates) such that maximum novel information about the underlying network is obtained in each experiment.
Choose an order that suits you best - by project, what to knit next, by weight, etc. Shuffle other books around on your bookshelf so that all your knitting books can be shelved together.
We choose an ordering of B such that ( m_1 le cdots le m_d).
(Chibrikov [90], see also [78], the CD-lemma for modules) Consider a non-empty set S ⊂ m o d k ⟨ X ⟩ ⟨ Y ⟩ with all s ∈ S monic and choose an ordering < on X ∗ Y as before.
We then choose an ordering Θ C ' in which x1 and x2 are neighbors and for which every two elements that were neighbors in C1 or C2 remain neighbors.
We find that the tensile instability can be suppressed by choosing an appropriate order of interpolation in the equation of motion of the Godunov SPH method.
Instead of choosing a market order, choose a stop limit order.
