Unterschiede
Hier werden die Unterschiede zwischen zwei Versionen angezeigt.
| Nächste Überarbeitung | Vorhergehende Überarbeitung | ||
| en:materialdaten:thermodynamische_daten [2024/04/11 15:20] – angelegt admin | en:materialdaten:thermodynamische_daten [2025/05/27 16:13] (aktuell) – neelest | ||
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| ======Thermodynamic data====== | ======Thermodynamic data====== | ||
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| + | ===== Material data - Thermodynamics ===== | ||
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| + | The rheological data of the material are entered in the ‘Thermodynamics’ tab: | ||
| + | * **Crystalline melting/ | ||
| + | * **Thermal conductivity**: | ||
| + | * **Molecular structure**: | ||
| + | * **Specific heat capacity**: This is only required for the melt. It is modelled as a straight line with a constant gradient with a value extrapolated to 0 °C ($c_{p,0}$) and a gradient of $c_{p,m}$ per 1 °C. | ||
| + | * **Melting enthalpy**: The enthalpy for melting the crystalline areas (only partially crystalline plastics) | ||
| + | * **Solids enthalpy**: The enthalpy up to the crystalline melting/ | ||
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| + | {{ : | ||
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| + | ===== Theoretical principles ===== | ||
| + | |||
| + | ==== Thermal conductivity ==== | ||
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| + | \[λ(T) = λ_0 + λ_m \cdot T\] | ||
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| + | $λ_0$ represents the thermal conductivity resulting from the straight line describing the melt range at 0 °C. The gradient of the thermal conductivity $λ_m$ 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. To determine this value, the thermal conductivity of the solid $λ_F$ must be entered. | ||
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| + | {{ : | ||
| + | ==== Specific heat capacity ==== | ||
| + | The function curve of the specific heat capacity $c_p$ at ambient pressure is shown for amorphous and semi-crystalline thermoplastics in the following figure. In the melt range, the specific heat capacity behaves almost linearly and can therefore be calculated using a linear equation: | ||
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| + | \[c_p(T) = c_{p,0} + c_{p, | ||
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| + | The peak in the curve for semi-crystalline thermoplastics describes the temperature $T_K$ and thus the melting temperature. | ||
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| + | {{ : | ||
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| + | ==== Specific Enthalpy ==== | ||
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| + | The specific enthalpy results from the integral of the specific heat capacity $c_p (T)$ | ||
| + | between the limits $T_1$ and $T_2$: | ||
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| + | \[Δh = \int \limits_ {T_1}^{T_2} c_p(T)dT\] | ||
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| + | This gives the amount of heat related to the unit mass that is required to increase the temperature of the polymer from $T_1$ to $T_2$. | ||
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| + | In contrast, semi-crystalline materials exhibit a step-like increase due to the phase transition. The additional amount of heat is referred to as the melting enthalpy $∆h_A$. The following figure shows the specific enthalpy as a function of temperature. | ||
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| + | {{ : | ||
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| + | When specifying an **amorphous thermoplastic**, | ||
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| + | Amorphous thermoplastics: | ||
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| + | Semi-crystalline thermoplastics: | ||
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| + | Plus the enthalpy increase in the melting range: $$∆h_{melt}=\frac{1}{2} c_{p,m} \cdot (T^2-{T_{K, | ||
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| + | ===Further topics=== | ||
| + | * [[en: | ||
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