Why is the strength of an elastomeric polymer network so low
- 1Department of Mechanical Engineering, Stanford University, Stanford, CA, USA
- 2Department of Management Science and Engineering, Stanford University, Stanford, CA, USA
- 3John A. Paulson School of Engineering and Applied Sciences, Harvard University, Boston, MA, USA
Abstract
Experiments have long shown that a polymer network of covalent bonds commonly ruptures at a stress that is orders of magnitude lower than the strength of the covalent bonds. Here, we investigate this large reduction in strength by coarse-grained molecular dynamics simulations. We show that the network ruptures by sequentially breaking only a small fraction of bonds, and that each broken bond lies on a path belonging to the left-tail of the “shortest paths” distribution. A shortest path is the path of the fewest bonds that connect two monomers at the opposite ends of the network. As the network is stretched, the strands along these left-tail shortest paths straighten and bear high tension set by covalent bonds, while most strands off these paths deform via entropic elasticity. After a bond on one of the left-tail shortest paths breaks, the load shifts to other left-tail shortest paths and the process repeats. As the network is stretched and bonds are broken, the scatter in lengths of the shortest paths first narrows, causing stress to rise, and then broadens, causing stress to decline. This sequential breaking of a small fraction of bonds causes the network to rupture at a stress that is orders of magnitude below the strength of the covalent bonds.
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BibTeX
@article{mohanty2026strength,
title = {{Why is the strength of an elastomeric polymer network so low}},
author = {Shaswat Mohanty and José Blanchet and Zhigang Suo and Wei Cai A},
journal = {npj Computational Materials},
year = {2026},
month = may,
doi = {10.1038/s41524-026-02143-5},
url = {https://doi.org/10.1038/s41524-026-02143-5},
note = {CC BY-NC-ND},
}
RIS
TY - JOUR
TI - Why is the strength of an elastomeric polymer network so low
AU - Shaswat Mohanty
AU - José Blanchet
AU - Zhigang Suo
AU - Wei Cai A
PY - 2026
DA - 2026/05/20
JO - npj Computational Materials
DO - 10.1038/s41524-026-02143-5
UR - https://doi.org/10.1038/s41524-026-02143-5
AB - Experiments have long shown that a polymer network of covalent bonds commonly ruptures at a stress that is orders of magnitude lower than the strength of the covalent bonds. Here, we investigate this large reduction in strength by coarse-grained molecular dynamics simulations. We show that the network ruptures by sequentially breaking only a small fraction of bonds, and that each broken bond lies on a path belonging to the left-tail of the “shortest paths” distribution. A shortest path is the path of the fewest bonds that connect two monomers at the opposite ends of the network. As the network is stretched, the strands along these left-tail shortest paths straighten and bear high tension set by covalent bonds, while most strands off these paths deform via entropic elasticity. After a bond on one of the left-tail shortest paths breaks, the load shifts to other left-tail shortest paths and the process repeats. As the network is stretched and bonds are broken, the scatter in lengths of the shortest paths first narrows, causing stress to rise, and then broadens, causing stress to decline. This sequential breaking of a small fraction of bonds causes the network to rupture at a stress that is orders of magnitude below the strength of the covalent bonds.
SN - 2057-3960
ER -