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Elasticity01:12

Elasticity

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Elasticity is the ability of an object to withstand the effects of distortion and to return to its original size and shape once the forces causing deformation are removed. When an elastic material deforms under the action of an external force, it experiences internal resistance to the deformation. However, if no external force is applied, it returns to its original state.
The elasticity of an object can be described by a stress-strain curve, which represents the relationship between stress...
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Elasticity in Concrete01:20

Elasticity in Concrete

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Upon subjecting concrete to moderate or high uniaxial compressive or tensile stresses, the strain response is non-linear relative to the stress applied. As the stress is removed, the resulting stress-strain curve deviates from the original path traced during loading, creating a hysteresis loop, indicative of the concrete's non-linear and non-elastic properties. Typically, a material's modulus of elasticity, which is a measure of the material's stiffness, is inferred from the linear...
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Elastic Potential Energy01:01

Elastic Potential Energy

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Elastic potential energy is the energy stored as a result of the deformation of an elastic object, such as the stretching of a spring. An object is elastic if it returns to its original shape and size after being deformed. 
Potential energy is also associated with the elastic force exerted by an ideal spring. The work done by this force can be represented as a change in the elastic potential energy of the spring. Thus, the work done by a perfectly elastic spring, in one dimension, depends...
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Strain and Elastic Modulus01:15

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The quantity that describes the deformation of a body under stress is known as strain. Strain is given as a fractional change in either length, volume, or geometry under tensile, volume (also known as bulk), or shear stress, respectively, and is a dimensionless quantity. The strain experienced by a body under tensile or compressive stress is called tensile or compressive strain, respectively. In contrast, the strain experienced under bulk stress and shear stress is known as volume and shear...
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Elastic Collisions: Introduction01:00

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15.2K
An elastic collision is one that conserves both internal kinetic energy and momentum. Internal kinetic energy is the sum of the kinetic energies of the objects in a system. Truly elastic collisions can only be achieved with subatomic particles, such as electrons striking nuclei. Macroscopic collisions can be very nearly, but not quite, elastic, as some kinetic energy is always converted into other forms of energy such as heat transfer due to friction and sound. An example of a nearly...
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Elastic Collisions: Case Study01:15

Elastic Collisions: Case Study

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Elastic collision of a system demands conservation of both momentum and kinetic energy. To solve problems involving one-dimensional elastic collisions between two objects, the equations for conservation of momentum and conservation of internal kinetic energy can be used. For the two objects, the sum of momentum before the collision equals the total momentum after the collision. An elastic collision conserves internal kinetic energy, and so the sum of kinetic energies before the collision equals...
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Related Experiment Video

Updated: Feb 11, 2026

Large Area Substrate-Based Nanofabrication of Controllable and Customizable Gold Nanoparticles Via Capped Dewetting
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Liquid dewetting under a thin elastic film.

Rafael D Schulman1, John F Niven, Michiel A Hack

  • 1Department of Physics and Astronomy, McMaster University, 1280 Main St. W., Hamilton, ON L8S 4M1, Canada. dalnoki@mcmaster.ca.

Soft Matter
|April 24, 2018
PubMed
Summary

We investigated liquid film dewetting under an elastomeric layer. Increasing elastomer tension slows hole growth, while biaxial tension creates non-circular holes, enabling shape control.

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Area of Science:

  • Materials Science
  • Fluid Dynamics
  • Polymer Physics

Background:

  • Dewetting of liquid films is crucial in various applications.
  • Elastomeric layers introduce tunable mechanical properties to thin films.
  • Understanding film rupture dynamics is key for material design.

Purpose of the Study:

  • To investigate the influence of elastomer tension on liquid film dewetting.
  • To explore the control of hole morphology and rim stability.
  • To demonstrate shape control of dewetting patterns via biaxial tension.

Main Methods:

  • Experimental study of liquid film dewetting.
  • Application of isotropic and biaxial tension to capping elastomeric layers.
  • Analysis of hole growth rates and morphology.

Main Results:

  • Isotropic tension in the elastomer reduces circular hole growth rate as tension increases.
  • Hole morphology and rim stability are controllable via boundary conditions and film tension.
  • Biaxial tension leads to non-circular holes elongated along the high tension axis.
  • Square-shaped holes were achieved with specific elastic boundary conditions.

Conclusions:

  • Elastomer tension significantly impacts liquid film dewetting dynamics.
  • Tunable control over dewetting patterns is achievable by manipulating elastomer stress.
  • This work offers insights into designing materials with controlled film rupture behavior.