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Second, the amplitude of a perturbation can eventually become unbounded in finite time, indicating flame quenching.
In other words, the solutions remain bounded while their slopes become unbounded in finite time.
As we shall see, under certain conditions the solutions of this problem can become unbounded in a finite time.
These solutions become unbounded in finite time at a single point at which there is a growing and increasingly narrow peak.
This is because we need to introduce more dual variables and because the constraint sets of the subproblems encountered in the dual domain become unbounded.
Here, may become unbounded for, the condition, or equivalently is not the correct condition for the solution to be continuous on.
Similar(40)
Obviously, becomes unbounded as, at the point.
Thus, the ratio in (22) becomes unbounded, contradicting the proper efficiency of (x^) for (P).
where is a non-negative parameter, and the function becomes unbounded at.
(g t,x)) being singular at 0 means that (g t,x)) becomes unbounded when (xrightarrow0^).
Obviously, ((underline{u}, underline{v})) becomes unbounded as (trightarrow T^) at the point (x=0).
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