@inproceedings{oai:jaxa.repo.nii.ac.jp:00007370, author = {奥泉, 信克 and 山本, 貴也 and Okuizumi, Nobukatsu and Yamamoto, Takaya}, book = {アストロダイナミクスシンポジウム講演後刷り集, Proceedings of 19th workshop on JAXA Astrodynamics and Flight Mechanics}, month = {Mar}, note = {アストロダイナミクスシンポジウム (2009年7月30-31日. 宇宙航空研究開発機構宇宙科学研究本部)), Workshop on JAXA Astrodynamics and Flight Mechanics, 2009 (July 30-31, 2009. Institute of Space and Astronautical Science (ISAS), Japan Aerospace Exploration Agency (JAXA)), Sagamihara, Kanagawa Japan, 膜面をしわを生じることなく円筒形状に折り畳むことのできるらせん折りを適用した六角形膜面について,真空槽内での遠心力展開実験を行い,多粒子系モデルによる数値シミュレーション結果と比較した.らせん折り膜面は遠心力によって滑らかに展開するが,展開後に面内・面外振動が発生することを示した.従来の多粒子系モデルに対し,座屈強度,空気抵抗,折り目剛性のシンプルなモデル化を追加し,また実験に合わせた初期形状の調整を行うことによって,数値シミュレーション結果が実験結果と概ね一致することを確認した., Centrifugal deployment dynamics of hexagonal membranes stowed with spiral folding are investigated. Centrifugal deployments have a possibility of unfolding large membranes without using extendable masts. Understanding and predicting the deployment dynamics are important to realize large membrane space structures. In this paper, deployment experiments of hexagonal membranes with coarse and fine spiral folding patterns are conducted in vacuum under gravity. Numerical simulations of the centrifugal deployments are also performed employing spring-mass system which models in-plane stiffness of thin membranes and enables fast numerical analysis. Modelings of buckling, creases, air drag and damping are added to the spring-mass system model and initial shapes are adjusted to experimental models. The experimental and numerical results are compared to examine the characteristics of the deployment dynamics and the validity of the numerical., 形態: カラー図版あり, Physical characteristics: Original contains color illustrations, 資料番号: AA0064734065}, publisher = {宇宙航空研究開発機構宇宙科学研究本部, Institute of Space and Astronautical Science, Japan Aerospace Exploration Agency (JAXA)}, title = {Experiments and Simulations of Centrifugal Deployments of Membranes Stowed with Spiral Folding}, volume = {2009}, year = {2010} }