Unterschiede
Hier werden die Unterschiede zwischen zwei Versionen angezeigt.
| Beide Seiten der vorigen RevisionVorhergehende ÜberarbeitungNächste Überarbeitung | Vorhergehende Überarbeitung | ||
| en:berechnungen:druckverlauf [2025/01/13 17:57] – neelest | en:berechnungen:druckverlauf [2025/07/03 13:34] (aktuell) – cschall | ||
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| ======Pressure profile====== | ======Pressure profile====== | ||
| - | The same conditions must be met for the calculation | + | -> [[en: |
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| + | To calculate | ||
| [[en: | [[en: | ||
| and [[en: | and [[en: | ||
| - | Additionally, | + | Additionally, |
| - | profile | + | The same equations as those used in the throughput |
| - | + | ||
| - | The pressure curve is calculated | + | |
| - | + | ||
| - | The pressure curve calculation starts at the screw tip. The calculated throughput is used to determine the pressure loss within a calculation interval and added to the previous absolute pressure. The pressure | + | |
| - | + | ||
| - | The pressure curve is calculated isothermally at the melt temperature in each step and then multiplied by a correction factor. From a physical point of view, this correction factor ensures that the calculation | + | |
| - | ==== Pressure | + | The pressure |
| - | In order to calculate | + | The pressure profile calculation begins at the screw tip. Based on the calculated throughput, |
| - | gradient has to be assumed. However, since every additional assumption increases | + | |
| - | inaccuracy, the so-called " | + | |
| - | assumption. Its calculation method is similar to the FEM calculation method. | + | |
| - | Here, single intervals are built for barrier flight, solid and melt channel and for each | + | ==== Pressure Profile Calculation |
| - | section between the individual balance points, the change in the flow is described by | + | |
| - | means of a linear equation. These equations form a linear system of equations. The | + | |
| - | equations only describe the development of the flow in the direction of the channel, | + | |
| - | which means that the mesh of the division of the geometry into the required intervals | + | |
| - | corresponds to constant conditions. | + | |
| - | {{ : | + | === Assumption of Equal Pressure Gradient === |
| + | Barrier screws can only be calculated analytically under the simplifying assumption of an equal pressure gradient in the melt and solid channels. Although this allows for rapid calculation, | ||
| - | Before the resulting equation system can be solved with the familiar algorithms used | + | === Network Calculation / Matrix Model === |
| - | to solve linear equation systems, it is first necessary to reduce the system. This | + | |
| - | reduction is achieved by allowing boundary conditions. | + | |
| - | {{ : | + | To eliminate the above-mentioned simplifying assumption, the so-called matrix model was additionally implemented. Its calculation process is similar to the FEM method, generating a mesh within the flow domain. The //Matrix Model// is an analogy model based on network theory from electrical engineering. |
| - | In the closed | + | This method is optionally available for barrier |
| - | last node in the channel direction, can be taken as being equal to zero. If an open | + | |
| - | barrier section is calculated, by contrast, it is sufficient | + | |
| - | in order to be able to calculate this design. Because of the lack of a geometrical | + | |
| - | separation, | + | |
| - | melt channel | + | |
| - | For a clear-cut solution of the system it is necessary to know about the mass flow. | + | A network |
| - | Here an iterative calculation helps, i.e. in the first step, the pressure-throughput | + | |
| - | behavior | + | |
| - | without considering the barrier section. In the second step, this throughput | + | |
| - | solve the equation system for the barrier section. Since the overall | + | |
| - | requirement | + | |
| - | individual screw sections, the calculated | + | |
| - | can be added to the pressure requirement of the remaining screw sections that was | + | |
| - | calculated in the first step. | + | |
| + | {{ : | ||
| - | ==== Pressure curve calculation | + | To solve the resulting system of equations, it must be reduced by incorporating boundary conditions. |
| + | For a closed barrier zone, the mass flow into the closed inlet or out of the closed outlet can be set to zero. For an open barrier section and for wave screws, due to the lack of separation at the beginning and end of the section, the pressure difference between the channels is set to zero. | ||
| - | The calculation of the pressure curve in wave zones is similar to the calculation of the //node point method// in barrier zones. The //node point method// is an analogue model of network theory from electrical engineering. | + | {{ : |
| - | A network is formed from the geometry of the screw, which is made up of simple geometries (rectangular channels). A //voltage source// (drag flow) and a resistance (pressure flow) are defined for each of these simple geometries. A matrix is created and solved from the network of stress sources and resistances so that, for a given pressure difference in the zone, not only the flow rate but also the pressure is obtained for each of the simple geometries, so that the pressure curve over the zone is also known. | + | |
| ===Further topics=== | ===Further topics=== | ||
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