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Ci-dessous, les différences entre deux révisions de la page.
| Les deux révisions précédentes Révision précédente Prochaine révision | Révision précédente | ||
| public:modeles:rotor_02:accueil [2022/09/16 10:18] – supprimée - modification externe (Unknown date) 127.0.0.1 | public:modeles:rotor_02:accueil [2023/04/21 15:20] (Version actuelle) – solenekojtych | ||
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| + | ====== Rotor 2 ====== | ||
| + | |||
| + | < | ||
| + | * [[# | ||
| + | * [[# | ||
| + | * | ||
| + | <pane id=" | ||
| + | |||
| + | <callout type=" | ||
| + | This model is not public, as there were problems in the computation of eigenfrequencies with code Aster (see the bottom of the page). | ||
| + | </ | ||
| + | |||
| + | ===== About ===== | ||
| + | |||
| + | |||
| + | Rotor 2 is part of a research program to study aspect ratio because the use of high aspect ratio blading can lead to a decrease in the axial length of compressors and therefore a reduction of their size and weight. To investigate the effects of aspect ratio on compressor range and efficiency, two transonic rotors (rotor 1 and 2) were designed and tested. The variation in aspect ratio was based on a change in aerodynamic chord, and the solidity was kept the same by varying the number of blades. | ||
| + | |||
| + | * Original technical report [(cite: | ||
| + | author | ||
| + | date = {1974}, | ||
| + | institution | ||
| + | title = {Performance of a transonic compressor rotor with an aspect ratio of 6.5}, | ||
| + | number | ||
| + | url = {https:// | ||
| + | } | ||
| + | </ | ||
| + | * Picture : | ||
| + | {{ : | ||
| + | < | ||
| + | |||
| + | |||
| + | <callout type=" | ||
| + | * {{ : | ||
| + | * {{ : | ||
| + | </ | ||
| + | |||
| + | |||
| + | |||
| + | ===== Reference blade ===== | ||
| + | |||
| + | The **reference blade** is defined with multiple-circular arc profiles[(cite: | ||
| + | |||
| + | |||
| + | ==== Geometry ==== | ||
| + | The geometry of rotor 2 is described in the [[https:// | ||
| + | {{ : | ||
| + | |||
| + | ==== Aerodynamic design | ||
| + | |||
| + | ^ ^ unit ^ value ^ | ||
| + | ^ pressure ratio | [-] | 1.53 | | ||
| + | ^ mass flow | ||
| + | ^ tip speed | ||
| + | ^ tip solidity | ||
| + | ^ aspect ratio | [-] | 6.5 | | ||
| + | ^ rotative speed | [rad/ | ||
| + | |||
| + | ==== Material properties | ||
| + | |||
| + | The material of rotor 2 is not defined in the original NASA report. A 200-grade maraging steel is considered: | ||
| + | |||
| + | ^ | ||
| + | ^ alloy | [-] | 18-Ni-200-maraging | ||
| + | ^ Young' | ||
| + | ^ density | ||
| + | ^ Poisson' | ||
| + | ^ yield stress | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | ==== CAD model ==== | ||
| + | |||
| + | The CAD model is computed with the open source code OpenMCAD[(cite: | ||
| + | |||
| + | < | ||
| + | <col md=" | ||
| + | </ | ||
| + | <col md=" | ||
| + | {{ : | ||
| + | < | ||
| + | </ | ||
| + | <col md=" | ||
| + | {{ : | ||
| + | < | ||
| + | </ | ||
| + | <col md=" | ||
| + | </ | ||
| + | </ | ||
| + | |||
| + | ==== Natural frequencies ==== | ||
| + | |||
| + | |||
| + | First three natural frequencies (with clamped root) for the mesh computed with OpenMCAD[(cite: | ||
| + | |||
| + | <callout type=" | ||
| + | Currently not available because of a problem to compute them with aster from the mesh of the reference blade. | ||
| + | </ | ||
| + | |||
| + | |||
| + | </ | ||
| + | |||
| + | <pane id=" | ||
| + | |||
| + | <callout type=" | ||
| + | Ce modèle n'est pas public, en raison de problèmes sur le calcul des fréquences propres avec code Aster (voir bas de page) | ||
| + | </ | ||
| + | |||
| + | ===== À propos ===== | ||
| + | |||
| + | Le rotor 2 fait partie d'un programme de recherche visant à étudier l’allongement des aubes, car l' | ||
| + | |||
| + | * Rapport technique original [(cite: | ||
| + | author | ||
| + | date = {1974}, | ||
| + | institution | ||
| + | title = {Performance of a transonic compressor rotor with an aspect ratio of 6.5}, | ||
| + | number | ||
| + | url = {https:// | ||
| + | } | ||
| + | </ | ||
| + | * Photographie : | ||
| + | |||
| + | {{ : | ||
| + | < | ||
| + | |||
| + | |||
| + | |||
| + | <callout type=" | ||
| + | * {{ : | ||
| + | * {{ : | ||
| + | </ | ||
| + | |||
| + | |||
| + | ===== Aube de référence ===== | ||
| + | |||
| + | L' | ||
| + | |||
| + | |||
| + | ==== Géométrie ==== | ||
| + | |||
| + | La géométrie du rotor 2 est décrite dans le [[https:// | ||
| + | |||
| + | {{ : | ||
| + | |||
| + | ==== Caractéristiques aérodynamiques | ||
| + | ^ ^ unités | ||
| + | ^ taux de compression | ||
| + | ^ débit massique | ||
| + | ^ vitesse en tête | [m/s] | 350,8 | | ||
| + | ^ solidité en tête | ||
| + | ^ allongement | ||
| + | ^ vitesse de rotation | ||
| + | |||
| + | |||
| + | ==== Propriétés matériau | ||
| + | |||
| + | Le matériau original du rotor 2 n'est pas défini dans le rapport de la NASA. Un acier maraging de grade 200 est considéré: | ||
| + | |||
| + | ^ | ||
| + | ^ alliage | ||
| + | ^ module d' | ||
| + | ^ masse volumique | ||
| + | ^ coefficient de Poisson | ||
| + | ^ limite élastique | ||
| + | |||
| + | ==== Modèle CAO ==== | ||
| + | |||
| + | < | ||
| + | <col md=" | ||
| + | </ | ||
| + | <col md=" | ||
| + | {{ : | ||
| + | < | ||
| + | </ | ||
| + | <col md=" | ||
| + | {{ : | ||
| + | < | ||
| + | </ | ||
| + | <col md=" | ||
| + | </ | ||
| + | </ | ||
| + | |||
| + | |||
| + | ==== Fréquences propres ==== | ||
| + | |||
| + | Fréquences des trois premiers modes (noeuds du pied d'aube encastrés) pour le maillage obtenu avec OpenMCAD[(cite: | ||
| + | |||
| + | <callout type=" | ||
| + | Il y a actuellement un problème sur le calcul des fréquences propres dans Aster. | ||
| + | </ | ||
| + | |||
| + | </ | ||
| + | </ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
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