Unterschiede
Hier werden die Unterschiede zwischen zwei Versionen angezeigt.
| Beide Seiten der vorigen RevisionVorhergehende ÜberarbeitungNächste Überarbeitung | Vorhergehende Überarbeitung | ||
| en:berechnungen:wandgleitende_materialien [2025/05/28 10:04] – neelest | en:berechnungen:wandgleitende_materialien [2026/07/14 09:55] (aktuell) – cschall | ||
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| - | ======Wall-slipping | + | ======Wall-slipping |
| - | The content is currently being processed | + | When considering flow processes in rheometers, but also in practical components such as dies, plasticizing units, |
| - | When considering | + | When the transition from wall adhesion to wall slip occurs, most equations used to calculate a flow are no longer valid. Since this is a very complex phenomenon that depends on viscosity, shear rate, shear stress, temperature, and pressure, a simple and stable empirical model is used. |
| - | such as dies, plasticating units and between gaps, the flowing melt is presumed | + | |
| - | wall adhering. In polymer melting | + | |
| - | However, there are some materials, among which the ultrahigh molecular | + | |
| - | polyethylene of high density (HDPE) | + | |
| - | (PVC, frequently provided with outward lubricants for a gentle processing), | + | |
| - | wall slipping under certain conditions. | + | |
| - | In order to calculate | + | Due to the complex relationships involved, |
| - | **PSI**, the option “wall slipping” has been added in the software. For this, critical | + | |
| - | Chapter Rheological Material Data. | + | |
| - | When choosing the menu item Wall slipping, **REX/PSI** considers that wall slipping | + | In REX/PSI, wall slip occurs above a critical shear stress. |
| - | occurs above the critical | + | |
| - | wall and the root surface are evaluated and limited to a value whose maximum is | + | |
| - | equal to the critical shear stress | + | |
| - | $$τ_ {WH,S} > τ_{krit} ⇒ τ_S = τ_{krit}$$ | + | For the dissipation calculation, the following applies: |
| - | This limitation has an effect on the flow profile in the screw channel and reduces the local pressure gradient. This reduces the pressure build-up capacity, but also the pressure consumption of | + | $$ \tau_0 = \eta_0 \cdot \dot{\gamma} $$ |
| - | screw zones that are passed over. | + | $$ if $$ |
| + | $$ \tau_0 > \tau_{crit}(T) $$ | ||
| + | $$ then $$ | ||
| + | $$ \Delta \tau = \tau_0 | ||
| + | $$ \tau_{target} = \tau_{crit}(T) + \Delta \tau \cdot k_{mat} $$ | ||
| + | $$ with $$ | ||
| + | $$ 0 < k_{mat} \leq 1 $$ | ||
| + | $$ it~follows~that $$ | ||
| + | $$ \eta_{wall~slipping} = \frac{\tau_{target}}{\dot{\gamma}} $$ | ||
| - | If a wall-sliding material | + | If the local shear stress |
| - | In addition, the material parameter $k_{mat}$ can be used to describe the increase in the dimensionless sliding velocity $V_{sl}^*$ as a function of the dimensionless shear stress $τ^*$. The required material data, such as the sliding velocity $v_{sl}$ as a function of the wall shear stress $τ$, is determined during the viscosity measurement (e.g. with a high-pressure capillary rheometer). | + | **Important: |
| - | During | + | If wall slip is checked in the material data, the values entered there are used. If wall slip is unchecked there, |
| - | {{ : | ||
| - | |||
| - | From the critical pressure $Δp_{krit}$ at which this discontinuity occurs, the critical wall shear stress $τ_{krit}$ can be calculated for a rectangular capillary using the following formula: | ||
| - | |||
| - | \[τ_{krit} = \frac{\Delta p_{krit}}{2} \frac{h}{l}\] | ||
| - | |||
| - | These critical shear stresses can be approximated as a straight line equation depending on the temperature. Therefore, **REX/PSI** requires the input of two pairs of values for the critical shear stress and the corresponding temperature. | ||
| ===Further topics=== | ===Further topics=== | ||