Exact(5)
Figure 6e,f show all proposed structures have small power stretch factors even when the network is very dense.
We show (for the case of Stokes flow) that designs with fewer baffles have comparable material stretch factors to corresponding designs with all baffles present.
As we expected, GG has a power stretch factor of one and all power stretch factors of 3D Yao structures are smaller than their theoretical bounds if they have ones.
Notice that Yao structures based on PYG8 and RNG have a little bit higher stretch factor than GG and other Yao-based structures, however, their maximum power stretch factors are still smaller than 5.
Results show that the mean turbulent flame stretch factors for lean/stoichiometric and rich mixtures were not equal when the unstrained premixed laminar burning velocity, non-dimensional bulk flow velocity, non-dimensional turbulence intensity, and non-dimensional longitudinal integral length scale were kept constant.
Similar(55)
The stretch factor was fun, too.
Thus, the stretch factor.
Hereafter, we call the Stretch Factor (SF).
Table 2 Stretch factor (SF) of LCSR (various sphere size).
Table 3 Stretch factor (CF) of CSR (various sphere size).
We also measure the Stretch Factor (SF) of CSR.
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