Unterschiede
Hier werden die Unterschiede zwischen zwei Versionen angezeigt.
| Beide Seiten der vorigen RevisionVorhergehende Überarbeitung | |||
| en:berechnungen:einrieselverhalten [2024/10/17 20:03] – [Feed section] neelest | en:berechnungen:einrieselverhalten [2025/01/20 10:56] (aktuell) – gelöscht cschall | ||
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| - | ======Feed section ====== | ||
| - | For the calculation of the feeding behavior the input of tribological and technological | ||
| - | data is required. | ||
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| - | **Realization of the theoretical principles** | ||
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| - | With regard to the processing the solid sections can be divided into three sections: | ||
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| - | I. Hopper and hopper opening | ||
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| - | II. Flow section without pressure built-up along the screw channel (∆p = 0) | ||
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| - | III. Conveying section with pressure built-up (∆p > 0) | ||
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| - | {{ : | ||
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| - | Most of the popular research and mathematical models focus on the third section ($∆p > 0$). This takes place among other things in case of a calculation with **REX/PSI** in | ||
| - | which the solid conveying is considered. | ||
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| - | In order to explain the data, the kinematic ratio in the screw channel is briefly set out | ||
| - | in the following: Usually the filling ratio $f$ of the screw refers to the volume of the | ||
| - | screw channel. Because of its geometrical shape the plastic pellet does not fill a | ||
| - | screw channel completely. Therefore the filling ratio can theoretically never be 1, | ||
| - | according to this definition. Here, the filling ratio is defined differently in order to | ||
| - | operate with the regularities used in the literature: | ||
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| - | $$f = \frac {\dot m_{spez} (n)} {\dot m_{spez 0} (n→0)}$$ | ||
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| - | First, the specific throughput ($\dot m_{spez}$, throughput per screw speed in [kg/ | ||
| - | constant with increasing screw speed and then continuously drops over the entire | ||
| - | rotational range. Only when the screw channels are completely filled the solid | ||
| - | conveying behavior is linear in the lower rotational range. | ||
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| - | In order to describe this decrease mathematically, | ||
| - | to the lower speed range (from the mathematical point of view this is the initial | ||
| - | increase of the throughput diagram). | ||
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| - | The following figure shows the development of the measured throughput speed behavior to | ||
| - | the filling ratio resulting from it. | ||
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| - | {{ : | ||
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| - | From the definition of the filling ratio, the following results for the calculation of the | ||
| - | throughput $\dot m$: | ||
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| - | $$\dot m (n) = f \cdot \dot m_{spez 0} \cdot n$$ | ||
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| - | According to this equation, in addition to the filling ratio function the specific | ||
| - | throughput $\dot m_{spez0}$ of the lower speed range has to be known for the calculation of | ||
| - | the throughput. In this case (completely filled screw channels, $f=1$, $Δp = 0$) the | ||
| - | following throughput relation applies: | ||
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| - | $$\dot m_{spez0} = \frac {\dot m}{n}|_{n→0} = ρ_s \cdot π \cdot D_a \cdot A_{quer} \cdot \frac {tan φ \cdot tan α}{tan α + tan φ}$$ | ||
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| - | with: $n$ = rotational speed, $ρ_s$ = bulk density, $D_a$ = diameter of the screw, $A_{quer}$ = channel cross section, $α$ = conveying angle, $φ$ = pitch | ||
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| - | Using the Schneider approach the conveying angle $α$ is calculated in the pressure | ||
| - | neutral case. | ||
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| - | Different possibilities to realise flow problems and solve them if necessary, are | ||
| - | offered to the user. This can be done by integration of the feed grooves or by | ||
| - | enlargement of the feed opening. It always has to be taken into consideration that the | ||
| - | issued results refer to the maximum throughput to be achieved. The following figure shows | ||
| - | how the present results can be combined with the plasticization. | ||
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| - | {{ : | ||
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| - | The blue curve (flow-dominated throughput) describes the maximally achievable | ||
| - | throughput on the basis of the feed conditions. Due to the fact that not more material | ||
| - | can arrive in the first screw sections, more polymer cannot be melted. The red curves | ||
| - | show the throughput behavior depending on the counterpressure. If no | ||
| - | counterpressure exists, the maximal throughput is achieved. The throughput behavior | ||
| - | is feed dependent. With increasing counterpressure the throughput is influenced with | ||
| - | regard to the counterpressure. Only with increasing counterpressure the feed | ||
| - | conditions must also be considered. Thus, the user can immediately decide whether | ||
| - | the pressure behavior of the screw is sufficient enough for compacting and melting | ||
| - | the solid. **Even if the throughput is flow-dominated, | ||
| - | pressure throughput e.g. for the melt behavior in REX/PSI is melt-dominated.** If | ||
| - | a calculation shall be conducted flow-dominatedly, | ||
| - | the processing parameters. | ||
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| - | ===Further topics=== | ||
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