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| en:materialdaten:thermodynamische_daten [2025/01/13 16:38] – neelest | en:materialdaten:thermodynamische_daten [2026/09/17 09:23] (aktuell) – gelöscht - Externe Bearbeitung (Unbekanntes Datum) 127.0.0.1 | ||
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| - | ======Thermodynamic data====== | ||
| - | ===== Input dialogue ===== | ||
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| - | The rheological data of the material are entered in the ‘Thermodynamics’ tab: | ||
| - | * **Crystallite melting/ | ||
| - | * **Thermal conductivity**: | ||
| - | * **Molecular structure**: | ||
| - | * **Specific heat capacity**: This is only required for the melting range. 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 $c_m$ per 1 °C. | ||
| - | * **Melting enthalpy**: The enthalpy for melting the crystalline areas (only partially crystalline plastics) | ||
| - | * **Solid enthalpy**: The enthalpy up to the crystallite melting/ | ||
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| - | {{ : | ||
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| - | ===== Theoretical principles ===== | ||
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| - | ==== 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 melting range at 0 degrees. The gradient of the thermal conductivity $λ_m$ can also be negative and must then be entered with a negative sign. The effective thermal diffusivity 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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| - | can be described. | ||
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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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| - | Semi-crystalline materials, on the other hand, exhibit a gradual increase due to the phase transformation. 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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| - | With indicating **amorphous thermoplastics** the field for melting enthalpy is not | ||
| - | editable. In case of **semi-crystalline thermoplastics** the increase in enthalpy $∆h$ is | ||
| - | formed by an enthalpy increase of the solid material $∆h_F$ and the melting enthalpy | ||
| - | $∆h_A$ : | ||
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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=== | ||
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