Related Experiment Video
Updated: Jan 29, 2026

07:30
Ensemble Force Spectroscopy by Shear Forces
Published on: July 26, 2022
1.9K
Force networks and jamming in shear-deformed sphere packings
H A Vinutha1,2, Srikanth Sastry1
1Jawaharlal Nehru Center for Advanced Scientific Research, Jakkur Campus, Bengaluru 560064, India.
Physical Review. E
|February 21, 2019
Summary
Shear jamming in granular matter becomes rigid at a critical contact number, D+1, regardless of friction. This jamming phenomenon aligns with frictionless systems, unifying descriptions of disordered matter rigidity.
Area of Science:
- Soft matter physics
- Granular mechanics
- Disordered systems
Background:
- Rigidity emergence in disordered particle assemblies is key in soft matter (gels, foams, granular matter).
- Shear jamming in frictional grains is a unique case where shear stress induces rigidity.
- Existing models for shear jamming lack integration with frictionless systems.
Purpose of the Study:
- To computationally analyze shear jamming conditions in frictionless sphere assemblies.
- To investigate the relationship between structural features and jamming in the absence of friction.
- To unify the understanding of jamming phenomena across diverse disordered matter.
Main Methods:
- Computational analysis of force and torque balance in sheared sphere assemblies.
- Validation using frictional simulations.
- Rigidity percolation analysis for 2D systems.
Main Results:
- Shear jamming occurs at a mean contact number Z = D+1 (for D=2,3), irrespective of friction, above random loose packing density.
- The shear jamming threshold aligns with the marginal stability condition for frictionless jamming.
- Rigidity percolation precedes shear jamming and coincides with over-constrained region percolation in 2D.
Conclusions:
- A geometric description of shear jamming is provided, linking it to frictionless jamming and glass transition concepts.
- This work helps develop a unified framework for jamming phenomenology in disordered matter.
- Identified an intermediate phase in shear jamming analogous to that in covalent glasses.
Related Concept Videos
Normal and Shear Force
3.3K
When a beam is subjected to different loads, such as weight, pressure, or other external forces, internal forces are generated within the beam. These forces can have a significant impact on the overall stability and strength of the structure. Engineers use various methods to analyze and determine the magnitude and direction of these internal forces. One common technique used to determine internal forces in beams is the method of sections. This method involves considering an imaginary point or...
3.3K
Network Covalent Solids
16.1K
Network covalent solids contain a three-dimensional network of covalently bonded atoms as found in the crystal structures of nonmetals like diamond, graphite, silicon, and some covalent compounds, such as silicon dioxide (sand) and silicon carbide (carborundum, the abrasive on sandpaper). Many minerals have networks of covalent bonds.
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
16.1K
Plastic Deformations
453
Plastic deformation represents a fundamental concept in materials science, which explains the irreversible change in the shape of a material when it experiences stress beyond its elastic capability. This phenomenon is important in structural engineering, especially in designing and analyzing cantilever beams—structures that are securely fixed at one end and bear loads at the opposite end. When these beams are subjected to loads within their elastic range, they will return to their...
453
Plastic Deformations
430
It is essential to understand how structural members behave under plastic deformation when the bending stress exceeds the material's yield strength. This state of deformation permanently alters the shape of the member, in contrast to the linear elastic behavior observed before yielding. The strain at any point in the member is expressed in terms of maximum strain. Notably, the neutral axis, which coincides with the centroid during elastic bending, shifts away from the centroid under plastic...
430
Protein Networks
4.5K
An organism can have thousands of different proteins, and these proteins must cooperate to ensure the health of an organism. Proteins bind to other proteins and form complexes to carry out their functions. Many proteins interact with multiple other proteins creating a complex network of protein interactions.
These interactions can be represented through maps depicting protein-protein interaction networks, represented as nodes and edges. Nodes are circles that are representative of a protein,...
These interactions can be represented through maps depicting protein-protein interaction networks, represented as nodes and edges. Nodes are circles that are representative of a protein,...
4.5K
Shear Diagram
1.6K
In the study of beam mechanics, shear diagrams play a crucial role in understanding the distribution of shear forces along the length of a beam. Consider a beam AB that is supported at both ends and subjected to perpendicular loads.
First, a free-body diagram of the beam is drawn, representing all the external forces and internal reactions acting on the beam. One can calculate the reaction forces at each support by employing the equilibrium equations of force and moment. The vertical component...
First, a free-body diagram of the beam is drawn, representing all the external forces and internal reactions acting on the beam. One can calculate the reaction forces at each support by employing the equilibrium equations of force and moment. The vertical component...
1.6K

