This paper reviews thoroughly available experiments and analytical approaches in the relevant international literature and introduces a calculation model for assessing steel bar mass loss and contributes to further utilization of common in-situ inspections from a structural point of view.
We introduce a flexible power calculation model that makes fewer simplifying assumptions, leading to a more accurate power analysis that can be used on a wide variety of study designs.
This methodology utilizes a modified Heliosat-2 model, and applies for all sky conditions; it also introduces a horizon calculation of the DTM points and accounts for the effect of snow covers.
A correlation between exposure dose and disease was obtained by introducing a modified calculation of morbidity, which can extend the assessment endpoint of health risk to disease burden from the conventional infection rate.
Afterwards, using the proposed model, we introduce a novel approach for the calculation of packet drop ratio, through which the negative effects of uncooperative nodes can be calculated.
By cutting off the parts of the observation uncertainty regions at these boundaries and not taking them into account for the center of gravity calculation, we introduce a slight bias towards the center of the rotation-velocity parameter space patch.
Here, we conservatively chose to not include in the model a term for endogenous biliary lead excretion into feces because endogenous fecal lead excretion is unknowable for a particular child, and including this term in the model would introduce a large uncertainty in the calculation of the bone lead contribution to blood.
Coupled with dynamic indoor load and actual operation characteristics of heat pump unit, a method to calculate actual dynamic heat load input of GHEs was introduced and a calculation program was developed.
To account for these effects, as well as other potential noise in the calculations, we introduce a tolerance on structure selection ∆Etol, and count the frequency with which PBE or SCAN erroneously stabilize a crystal structure by more than ∆Etol with respect to the experimental ground state structure.
Since diffusion is fast within each grid (∼1 s), this choice of grid size is unlikely to introduce a notable error in our calculations.
