The end of year result based on input/output calculation was Cte = Cti + It − Ot of Cl.
The end of year result based on input/output calculation was Cte = Cti + It − Ot, which is the total estimated Cl mass at the end of year based on the conservation of mass.
There is also a dummy (μ t ) representing general change between the time points, and an error term, ε cti.
This is accomplished by adding cross-product terms (e.g., α2 (U ct × Gender cti )) to the equation.
The charge transfer between ions of Si and C atoms is denoted in terms of a force parameter f cti and is expressed as [20, 21, 22]: f_{text{cti}} = f_{0} exp ( - r/rho ) (11).
The phase stability of cubic 3C SiC under high pressures is essentially based on material parameters namely hardness (b), range, non-central many body forces as charge transfer force (f cti) and covalency parameter (f cov).
(1, 2) is an algebraic sum of non-central many-body forces as the charge transfer force parameter and the force parameter arises due to covalent nature, i.e., f(r) = f cti + f cov.
Deduced values of hardness (b), range parameter, and non-central many body forces arising due to charge transfer (f cti) and covalency (f cov) for 3C SiC ceramics are illustrated in Table 1.
The charge transfer between ions of Si and C atoms is denoted in terms of a force parameter f cti and is expressed as [27, 33, 34]: f_{cti} = f_{0} exp ( - r/rho ) (11).
The computed strontium SrX (X = O, S, Se, and Te) chalcogenides, material parameter of hardness (b), range, and non-central many-body forces arose due to charge transfer (f cti) and covalency (f cov) for SrX is illustrated in Table 1.
