Diese Seite ist nicht editierbar. Sie können den Quelltext sehen, jedoch nicht verändern. Kontaktieren Sie den Administrator, wenn Sie glauben, dass hier ein Fehler vorliegt. ====== Thermal Conductivity ====== ===== Thermal Conductivity ===== **Path:** Main menu > Material > New polymer... Tab: Thermodynamic Data\\ {{:materialdaten:reine_polymere_uebersicht:iconmaterialnew-material.ico?nolink&60x60 |}} \\ \\ \\ **Path:** Main menu > Material > Edit material (file)... Tab: Thermodynamic Data\\ {{:materialdaten:reine_polymere_uebersicht:iconmaterialedit-material.ico?nolink&60x60 |}} \\ \\ \\ {{ :en:materialdaten:reine_polymere_uebersicht:thermodynamische_daten:en_sigma150_dlg_materialdaten_002.png?nolink |}} **Figure:** Dialog box Thermodynamic data In the case of thermal conductivity, it is necessary to distinguish between steady-state and non-steady-state temperature fields. With steady-state temperature fields, only the thermal conductivity l is available as a material value. This is temperature-dependent and higher for semi-crystalline materials than for amorphous ones, see figure. Thermal conductivity: $\lambda(T) = \lambda_0 + \lambda_m \cdot T$ {{ :en:materialdaten:reine_polymere_uebersicht:thermodynamische_daten:en_sigma150_dlg_materialdaten_005.svg?nolink&700 |}} **Figure:** Thermal conductivity as a function of temperature The value $\lambda_0$ which has to be entered represents the value obtained from the straight line that describes the molten range at 0 degrees. The gradient for the thermal conductivity can also be negative and must then be entered with a negative sign. The effective thermal conductivity of the solid is required for the melting calculation. For purposes of determining this value, it is necessary to enter the thermal conductivity of the solid. The melting point $T_{k,g}$ must also be entered on this mask. In the case of semi-crystalline materials, this temperature is interpreted as the crystalline melting point $T_k$ and in the case of amorphous polymers, as the glass transition point $T_g$ .