PMC:4534144 / 7639-9306
Annnotations
{"target":"https://pubannotation.org/docs/sourcedb/PMC/sourceid/4534144","sourcedb":"PMC","sourceid":"4534144","source_url":"https://www.ncbi.nlm.nih.gov/pmc/4534144","text":"Incinerator simulation\nTo simulate the studied incinerator, a Cartesian coordinate system with the dimensions of 20 × 20 × 20 mm containing 10,424 control volumes was used. The x, y and z axes represent the length, width and height, respectively [24]. In the regions where sharp gradients in the variables are expected, fine meshing is considered as possible. Structured meshes were used for meshing the model, because the number and distribution of meshes in different solution regions can be controlled. In addition, the boundary conditions can be well defined [24]. The boundary layer mesh generator was used in the regions where thermal analysis was important. Fig. 1a and b show the model, the meshed model and boundary conditions.\nFig. 1 a A view of the meshed model of the incinerator, (b) The geometrical charactersitics of the incinerator and boundary conditions\nWall boundary condition was considered on the studied incinerator, because the solid surface is in direct contact with the fluid [24]. Given that the size and profile of the inlet pressure to the studied incinerator are known, the pressure inflow and pressure outflow were selected for inlet and outlet boundary conditions, respectively. The walls were made of steel with a thermal conductivity of 202 W/M.K. For the flows with a velocity less than the speed of sound, a turbulence of less than 5 % can be considered as assumed in the present model. Other inputs are described in Table 2.\nTable 2 The inputs to the Fluent model\nValue Parameter\n3 % Turbulent Intensity\nStationary Wall Motion\nNo slip Shear Condition\n0.00004 (m) Roughness Height\n2.76 (m) Hydraulic Diameter\n0.5 Roughness Constant","divisions":[{"label":"title","span":{"begin":0,"end":22}},{"label":"p","span":{"begin":23,"end":872}},{"label":"figure","span":{"begin":737,"end":872}},{"label":"label","span":{"begin":737,"end":743}},{"label":"caption","span":{"begin":744,"end":872}},{"label":"p","span":{"begin":744,"end":872}},{"label":"label","span":{"begin":1462,"end":1469}},{"label":"caption","span":{"begin":1470,"end":1500}},{"label":"p","span":{"begin":1470,"end":1500}},{"label":"tr","span":{"begin":1501,"end":1516}},{"label":"th","span":{"begin":1501,"end":1506}},{"label":"th","span":{"begin":1507,"end":1516}},{"label":"tr","span":{"begin":1517,"end":1540}},{"label":"td","span":{"begin":1517,"end":1520}},{"label":"td","span":{"begin":1521,"end":1540}},{"label":"tr","span":{"begin":1541,"end":1563}},{"label":"td","span":{"begin":1541,"end":1551}},{"label":"td","span":{"begin":1552,"end":1563}},{"label":"tr","span":{"begin":1564,"end":1587}},{"label":"td","span":{"begin":1564,"end":1571}},{"label":"td","span":{"begin":1572,"end":1587}},{"label":"tr","span":{"begin":1588,"end":1616}},{"label":"td","span":{"begin":1588,"end":1599}},{"label":"td","span":{"begin":1600,"end":1616}},{"label":"tr","span":{"begin":1617,"end":1644}},{"label":"td","span":{"begin":1617,"end":1625}},{"label":"td","span":{"begin":1626,"end":1644}},{"label":"td","span":{"begin":1645,"end":1648}}],"tracks":[]}