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The strain-life method was used to determine the time required for crack initiation, while Paris' law was used to obtain the time required for the crack to grow from initial crack size to the critical value.
In this stage, gel viscosity rose rapidly from initial value to the maximum value.
The initial yield strength is nearly independent of the hydrostatic pressure but the strain hardening rate increases with stress triaxiality up to a critical value.
However, initial ratios below the critical value ϕ G, c will not converge to ϕ G *. Other interactions (, and ) do not converge to a stable ratio.
They tightened the critical value to 2.195
We see from Theorem 1.2 in [18] that the critical value about the initial data for global existence of (1.1) with (lambda_{1}=0) and (1.1) is the same.
When n >m the initial magnitude of CB must exceed a critical value if a subsequent increase in CB is to occur.
This critical value is shown to depend on the initial value of CA and on Vo.
The prevalence, C t), and its critical value, Cm, are normalized to the initial population size.
Likewise, the precise critical value for the block will differ from cell to cell.
This critical value of μBax for the transition from bistability to monostability is called a limit point.
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