People | Locations | Statistics |
---|---|---|
Naji, M. |
| |
Motta, Antonella |
| |
Aletan, Dirar |
| |
Mohamed, Tarek |
| |
Ertürk, Emre |
| |
Taccardi, Nicola |
| |
Kononenko, Denys |
| |
Petrov, R. H. | Madrid |
|
Alshaaer, Mazen | Brussels |
|
Bih, L. |
| |
Casati, R. |
| |
Muller, Hermance |
| |
Kočí, Jan | Prague |
|
Šuljagić, Marija |
| |
Kalteremidou, Kalliopi-Artemi | Brussels |
|
Azam, Siraj |
| |
Ospanova, Alyiya |
| |
Blanpain, Bart |
| |
Ali, M. A. |
| |
Popa, V. |
| |
Rančić, M. |
| |
Ollier, Nadège |
| |
Azevedo, Nuno Monteiro |
| |
Landes, Michael |
| |
Rignanese, Gian-Marco |
|
Berfield, Thomas A.
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (5/5 displayed)
- 2023Compressive creep buckling of single cell metamaterial at elevated temperatures
- 2022Residual stresses in additively manufactured parts: predictive simulation and experimental verificationcitations
- 2018Influences of Printing Parameters on Semi-Crystalline Microstructure of Fused Filament Fabrication Polyvinylidene Fluoride (PVDF) Components
- 2018A MEMS-scale vibration energy harvester based on coupled component structure and bi-stable states
- 2003Residual Stress Effects in Ferroelectric Thin Filmscitations
Places of action
Organizations | Location | People |
---|
article
Compressive creep buckling of single cell metamaterial at elevated temperatures
Abstract
<jats:title>Abstract</jats:title><jats:p>The benefits of tailored lattice topologies are limited in elevated temperature conditions without a clear understanding about the interplay between the metamaterial structure and the creep response of the base material. This study showed that the metamaterial structure causes the lattice compressive creep behavior to differ largely from that of bulk structures of the same base material. Inconel 625 FCCZ lattices and solid round bar specimens were crept in compression at two elevated temperatures and at three stress levels. The solid round bar specimens experienced only small increases in the steady state creep rate with a steady state exponent of 0.35 and 0.63 at 550°C and 650°C. The solid round bar specimens did not exhibit a deformation mechanism change over the temperatures and stress levels tested. The FCCZ lattices exhibited much larger changes in creep rates with changing stress and temperature with a steady state exponent of 18.3 and 20.2 at 550°C and 650°C, respectively. Additionally, the lattice specimens experienced three different failure behaviors with increasing temperature and stress from stable creep, to progressive buckling, and finally rapid collapse.</jats:p>