Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil....
Transcript of Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil....
![Page 1: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/1.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Problem 4Origami Launcher
Reporters: Matheus Pessôa, Lucas Maia
Team Brazil: Andrius D., André Juan, Gustavo Saraiva, Henrique Ferreira, Lucas Maia, Lucas Tonetto, Matheus Pessôa, Ricardo Gitti
1
Team Brazil
![Page 2: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/2.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
The problem
oFolded paper structures such as the Miura-oriorigami can be programmed to exhibit a wide rangeof elastic properties depending on their creaseand defect patterns. Design and build an origamicannon to vertically launch a standard Ping-Pongball using only a single uncut sheet of A4 paper(80g/m²). How is the height of the ball elevationrelated to the folding pattern? Optimize yourdesign to achieve the maximum height possible.
2
![Page 3: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/3.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Metamaterials
oOrigami metamaterials display, for example, auxetic behavior and multistability, the latter allowing reprogrammable configurations [3].
3
1. Flower petals 2. Insect wings
Images: 1. https://www.dreamstime.com/stock-photo-wings-insect-isolated-white-background-clipping-path-image72794552
2. https://www.asianscientist.com/2014/10/in-the-lab/making-3d-metamaterials-natural-bent/3. PRL 2016, V. Brunck,Elastic theory of origami-based metamaterials
[1] [2]
![Page 4: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/4.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Behavior of metamaterials
oContraction and dilation of the system
4
oMovement in a given direction is reflectedtowards another direction
Image: https://materia.nl/article/toolkit-build-reconfigurable-metamaterials/
3. Configurable metamaterial
![Page 5: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/5.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Investigating Miura-Ori patterns
5Image: Jesse L. Siverberg - “Using origami design principles to fold reprogrammable mechanical metamaterials”
4. 3D reconstruction of Miura-Ori
Patterns with geometric parameters
oGeometrical construction
oBased on creases and valleyso Can be characterized accordingly to different
geometric angles and properties
oVery important: Poisson’s ration!
![Page 6: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/6.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Poisson’s ratio- Why it is important
oFrom the references [1], we have that the origami’s Poisson’s ratio isnegative!
oTherefore, it is an auxetic material
6Reference [1], Image 6- Z.Y. Wei- “Geometric Mechanics of Periodic Pleated Origami”
Image 5- https://groups.exeter.ac.uk/auxetic/auxetic_f2.html
5. Behavior of an auxetic material
𝑣 = −𝑊
𝐿
𝑑𝐿
𝑑𝑊
𝑣 = 𝑃𝑜𝑖𝑠𝑠𝑜𝑛′𝑠 𝑟𝑎𝑡𝑖𝑜𝑊 = 𝑐ℎ𝑎𝑛𝑔𝑒 𝑖𝑛 𝑤𝑖𝑑𝑡ℎ𝐿 = 𝑐ℎ𝑎𝑛𝑔𝑒 𝑖𝑛 𝑙𝑒𝑛𝑔𝑡ℎ
𝑬𝒒𝒖𝒂𝒕𝒊𝒐𝒏𝒔
𝒗 = 𝟏 −𝟏
𝒔𝒆𝒏 𝜶 𝒔𝒆𝒏𝜽𝟐
Theoretical prediction for Miura-Ori
6. 3D modelling for Miura-Ori pattern
General case
![Page 7: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/7.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Negative Poisson’s ratio- evidence
7
7. Experiments for Miura-Ori patterns confirming the
negative Poisson’s ratio.
Image 7: Jesse L. Siverberg - “Using origami design principles to fold reprogrammable mechanical metamaterials”
o Justifies the choosing of a Miura-Oripattern for our investigations
oNow focusing on the problem itself
Achieving maximum
heights with a Miura-Ori
![Page 8: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/8.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Energy on a Miura-Ori origami
8
𝑼
𝒌𝟎𝒍=𝟏
𝟐𝜽+ − 𝜽𝟎
𝟐 +𝟏
𝟐𝜽− + 𝜽𝟎 − 𝟐𝝅 𝟐 + 𝜷 − 𝜷𝟎
𝟐 + 𝝓− 𝝅 𝟐
𝑬𝒒𝒖𝒂𝒕𝒊𝒐𝒏𝒔
𝑙 = 𝑓𝑜𝑙𝑑 𝑙𝑒𝑛𝑔ℎ𝑡𝑘0 = 𝑠𝑝𝑟𝑖𝑛𝑔 𝑐𝑜𝑛𝑠𝑡𝑎𝑛𝑡
Applied Angular Hooke’s law
8. Angular schemes
for a Miura-Ori folding
pattern
Non-dimensional approximation of the Energy behavior
Image 8: Jesse L. Siverberg - “Using origami design principles to fold reprogrammable mechanical metamaterials”
Our model also
considerspattern deffects!
![Page 9: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/9.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Energy on a Miura-Ori origami
9
𝑼
𝒌𝟎=𝒍
𝟐𝜽+ − 𝜽𝟎
𝟐 + 𝜽− + 𝜽𝟎 − 𝟐𝝅 𝟐 + 𝟐 𝜷 − 𝜷𝟎𝟐
𝑬𝒒𝒖𝒂𝒕𝒊𝒐𝒏𝒔
𝑙 = 𝑓𝑜𝑙𝑑 𝑙𝑒𝑛𝑔ℎ𝑡𝑘0 = 𝑠𝑝𝑟𝑖𝑛𝑔 𝑐𝑜𝑛𝑠𝑡𝑎𝑛𝑡𝑛 = 𝑛𝑢𝑚𝑏𝑒𝑟 𝑜𝑓 𝑐𝑟𝑒𝑎𝑠𝑒𝑠𝐶 = 𝑛𝑢𝑚𝑏𝑒𝑟 𝑜𝑓 𝑐𝑜𝑙𝑢𝑚𝑛𝑠
o 𝑙 can be varied experimentally
o 𝒌𝟎 is constant for all experiments, same 80 𝑔
𝑐𝑚2 uncut sheef ot paper
o Variation in (𝑙 ∗ 𝑎𝑛𝑔𝑙𝑒) implies angular changes
o Different energies → different heights!
![Page 10: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/10.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Experimental considerations
oMiura-Ori with 4 different number of foldso 5,6, 8 ,16 folds
10
56
8 16
![Page 11: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/11.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Angle measurements (𝜽𝟎, 𝝓, 𝜷𝟎, 𝜽+, 𝜽−)
117 folds 16 folds
6 folds5 folds
![Page 12: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/12.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Experimental considerations
oEnergy conversion𝑼𝒊 = 𝑼𝒇
𝑼𝒊
𝒌𝟎= 𝒍
𝟏
𝟐𝜽+ − 𝜽𝟎
𝟐 +𝟏
𝟐𝜽− + 𝜽𝟎 − 𝟐𝝅 𝟐 + 𝜷− 𝜷𝟎
𝟐 + 𝝓− 𝝅 𝟐
Theoretically, we expect a linear behavior of𝑼𝒊
𝒌𝟎in function of 𝑼𝒇!
12
𝑼𝒇 = 𝒎𝒈𝒉
![Page 13: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/13.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Proof of angular importance on the problem
13
o Linear behavior is comproved for thesefour origamis!
𝛼 ≅ (9.6 ± 0.4)𝑎. 𝑢.
𝐴ℎ
![Page 14: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/14.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Helicoidal model
oAnother way to build an origami pattern!
14
1 full step
Measurement of a full step in centimeters
![Page 15: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/15.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Helicoidal model
oPlotting results for the helicoidal model
15
o Quadratic fit!
o Explanation: a direct conversion of energy from the elastic one stored in the origami (completely) into the height of the ball!
𝑦 = 𝑦0 + 𝐵1𝑥 + 𝐵2𝑥2
𝐵1 = (39.63446 ± 0.465)
𝐵2 = (−1.3313 ± 0.01)
![Page 16: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/16.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Distribution for both experimental models
16
![Page 17: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/17.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
All experimental results
17
![Page 18: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/18.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Heights achieved with all origamis
18
![Page 19: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/19.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Summary
19
Miura-ori geometryExperiments Linear fit for results!Energy
Helicoid model
Maximized jump: helicoid model with step size of 15 cm!
𝒉𝑨 ~ 𝟐𝟔 ± 𝟎. 𝟎𝟓 𝒄𝒎
Quadratic fit due to
elastic properties
![Page 20: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/20.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
References
o [1] - Image https://www.dreamstime.com/stock-photo-wings-insect-isolated-white-background-clipping-path-image72794552
o [2] Image- https://www.asianscientist.com/2014/10/in-the-lab/making-3d-metamaterials-natural-bent/
o [3] PRL 2016, V. Brunck,Elastic theory of origami-based metamaterials
20
![Page 21: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/21.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Appendix
21
![Page 22: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/22.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Distribution for all Miura-Ori results
22
![Page 23: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/23.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
Experimental results for both designs
23
![Page 24: Apresentação do PowerPointiptnet.info/wp-content/uploads/2018/11/X-4-Br.pdf · 1 Team Brazil. Team Brazil Introduction Experiments Conclusion Origami Launcher The problem oFolded](https://reader034.fdocuments.us/reader034/viewer/2022050213/5f5f892108d0895e8549ba4b/html5/thumbnails/24.jpg)
Team
Brazil
Introduction
Experiments
Conclusion
Origami
Launcher
24