Steady-State Three - Dimensional Numerical Simulation of Heat Transfer for Thermal Bridges Assessment

Abstract

C 12 H 22 CdN4O14, triclinic, P¯ (no. 2), a = 7.188(2) Å, b = 8.895(3) Å, c = 9.771(3) Å, α = 63.148(3)°, β = 76.750(3)°, γ = 66.225(3)°, V = 509.2(3) Å 3 , Z = 1, Rgt(F) = 0.0253, wR ref (F 2 ) = 0.0676, T = 296(2) K. CCDC no.: 1484775The crystal structure is shown in the gure. Tables 1 and 2 contain details of the measurement method and a list of the atoms including atomic coordinates and displacement parameters. Source of materialThe title compound was synthesized by a hydrothermal method under autogenous pressure. A mixture of CdCl 2 ·H 2 O

Development of Methods and Algorithms for Estimating the Temperature Distribution in the Body of a Rectangular Parallelepiped Shape Under the Influence of Heat Flow and the Presence of Heat Exchange

“…In [16], one computational approach to the calculation of the heat equation is presented, which differs in the case of three-dimensional oblique unstructured grids by the compactness of the grid pattern and the unconditional stability of the numerical algorithm. The work [17] is part of a broader study on the assessment of heat transfer through the elements of building enclosing structures by the most accurate assessment of the effect of thermal bridges of the most common building structures. Currently, the discontinuous Galerkin method with discontinuous basis functions is widely used in [18], which is characterized by a high order of accuracy of the resulting solution.…”