High‐Strength, Thermally Activated Shape Memory Hydrogels Based on Hydrogen Bonding between MAAc and NVP

2018 ◽  
Vol 219 (10) ◽  
pp. 1700636 ◽  
Author(s):  
Chao Xu ◽  
Quan Tang ◽  
Haiyang Yang ◽  
Kang Peng ◽  
Xingyuan Zhang
2015 ◽  
Vol 3 (30) ◽  
pp. 6347-6354 ◽  
Author(s):  
Zongqing Ren ◽  
Yinyu Zhang ◽  
Yongmao Li ◽  
Bing Xu ◽  
Wenguang Liu

Diaminotriazine hydrogen bonding reinforced and Ca2+-crosslinked high strength shape memory hydrogels are fabricated. Ca2+_induced dramatic volume shrinkage is utilized to trigger unharmful cell detachment.


Author(s):  
Yufang Song ◽  
Yiming Chen ◽  
Ran Chen ◽  
Hongji Zhang ◽  
Dongjian Shi ◽  
...  

2020 ◽  
Vol 28 ◽  
pp. 2110-2117
Author(s):  
Fedor S. Belyaev ◽  
Margarita E. Evard ◽  
Eugeny S. Ostropiko ◽  
Aleksandr E. Volkov

2021 ◽  
Vol 245 ◽  
pp. 112827
Author(s):  
Mohammadreza Izadi ◽  
Masoud Motavalli ◽  
Elyas Ghafoori

Author(s):  
Daseul Jang ◽  
Chase B. Thompson ◽  
Sourav Chatterjee ◽  
LaShanda T. J. Korley

This paper highlights the influence of peptide secondary structure on the shape memory behaviour of peptidic polyureas, driven by hydrogen bonding arrangement and microphase-separated morphology.


2008 ◽  
Vol 106 (6) ◽  
pp. 630-640 ◽  
Author(s):  
V. V. Sagaradze ◽  
V. I. Voronin ◽  
Yu. I. Filippov ◽  
V. A. Kazantsev ◽  
M. L. Mukhin ◽  
...  

2011 ◽  
Vol 78 (6) ◽  
Author(s):  
Richard V. Beblo ◽  
Lisa Mauck Weiland

Presented are the experimental results of two light activated shape memory polymer (LASMP) formulations. The optical stimulus used to activate the materials is detailed including a mapping of the spatial optical intensity at the surface of the sample. From this, results of energy calculations are presented including the amount of energy available for transitioning from the glassy state to the rubbery state and from the rubbery state to the glassy state, highlighting one of the major advantages of LASMP as requiring less energy to transition than thermally activated shape memory polymers. The mechano-optical experimental setup and procedure is detailed and provides a consistent method for evaluating this relatively new class of shape memory polymer. A chemical kinetic model is used to predict both the theoretical glassy state modulus, as only the sample averaged modulus is experimentally attainable, as well as the through thickness distribution of Young’s modulus. The experimental and model results for these second generation LASMP formulations are then compared with earlier LASMP generations (detailed previously in Beblo and Mauck Weiland, 2009, “Light Activated Shape Memory Polymer Characterization,” ASME J. Appl. Mech., 76, pp. 8) and typical thermally activated shape memory polymer.


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