However, when the image has limited size, as it is common in practice, the estimate from a ACF-based algorithm is biased due to the mismatch of image intensities at the boundaries: the maximum point of ACF, which determines the estimated value, is slightly shifted from the exact value.
Since harmonic functions that are continuous to the boundary satisfy the maximum principle [17], we obtain the uniqueness by the standard argument for linear differential equations satisfying the maximum principle.
For a range of the proximity parameter γ (the ratio of the distance the bubble is created from the boundary to the maximum bubble radius), we record the impulsive forces generated by the bubble collapse.
Under the same boundary conditions, the maximum torque pro- duced by the proposed biomimicry turbine at zero rotational speed is 38.71 Nm which is 1110% greater than the torque generated by the turbine of Bahaj et al.
The position of maximum ECE was found in the vicinity of nonergodic and ergodic phase boundary, where the maximum change in entropy occurs as a result of the field induced phase transformation between the ergodic and long range ferroelectric phase.
It is also found that under a uniform upstream boundary condition, the maximum difference in mass flow rate between the fuel assemblies is less than 2%, while it slightly increases to 2.3% under a non-uniform condition.
The maximum tangential residual stresses occur at the boundaries, while the maximum radial residual stresses are near the mean radius.
The smaller cell interior sizes and thicker cell walls result in a greater contribution of grain interior to strengthening of polycrystalline material than the grain boundaries, with the maximum effect observed at 673 K due to dynamic strain aging.
For and using Dunnett critical boundaries for the maximum type 1 error rate is still inflated up to 0.0545, but interestingly the inflation is smaller compared to.
