Sentence examples for contribution of branch from inspiring English sources
It is achieved by introducing an auxiliary state vector: {varvec{y}} = { U_{i},K_{ij},L_{ij} } (4 where ( varvec{y} in R^{N + 2b} ) is the auxiliary state vector; N the number of buses; b the number of branches; U i = v i 2 the square of voltage magnitude; and K ij = v i v j cos θ ij and L ij = v i v j sin θ ij the contribution of branch ij (from bus i to bus j) to y.
To confirm the contribution of branch elimination to dendrite configuration in vivo, we performed time-lapse observation using an organotypic culture in which the cortical cytoarchitecture of the cerebellum was at least partly retained.
Reduced frequency of intermediate branches in RBP KO resin casts was due in part to branch loss, as demonstrated by a reduction in segment number with age, but we cannot rule out the contribution of branch shortening to the phenotype (Fig. 5A,B).
Despite the pivotal contribution of branching pattern innovations to the evolution of plant architecture, the mechanisms underlying the evolution of branching are poorly understood (Sussex and Kerk, 2001).
The hydrodynamics are assumed to be purely linear, i.e. viscous laminar flow is assumed everywhere, inertial effects and non-linear contributions of branching singularities are neglected.
Furthermore, the coefficient matrices entering the solution scheme are obtained by assembling the separate contribution of each branch, thus avoiding the ad hoc node numbering and branch orientation required by alternative implementations.
The contribution of LA branch is length and roughness insensitive.
The contribution of TA branch to thermal conductivity increases with increasing the length or decreasing the edge roughness of GNRs.
On the contrary, the contribution of ZA branch to thermal conductivity increases with decreasing the length or increasing the edge roughness of GNRs.
By incorporating the direction dependent phonon boundary scattering into the linearized phonon Boltzmann transport equation, we find that because of lower Grüneisen parameter, the TA phonons have the major contribution to thermal conductivity of GNRs, and in the case of smooth edge and micron length of GNRS, the relative contribution of TA branch to thermal conductivity is over 50%.
The present paper is aimed at establishing the framework of this unification tentative, highlighting the contribution of each branch.
