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Related Concept Videos

Damped Oscillations01:07

Damped Oscillations

In the real world, oscillations seldom follow true simple harmonic motion. A system that continues its motion indefinitely without losing its amplitude is termed undamped. However, friction of some sort usually dampens the motion, so it fades away or needs more force to continue. For example, a guitar string stops oscillating a few seconds after being plucked. Similarly, one must continually push a swing to keep a child swinging on a playground.
Although friction and other non-conservative...
Types of Damping01:20

Types of Damping

If the amount of damping in a system is gradually increased, the period and frequency start to become affected because damping opposes, and hence slows, the back and forth motion (the net force is smaller in both directions). If there is a very large amount of damping, the system does not even oscillate; instead, it slowly moves toward equilibrium. In brief, an overdamped system moves slowly towards equilibrium, whereas an underdamped system moves quickly to equilibrium but will oscillate about...
Second Order systems II01:18

Second Order systems II

In an underdamped second-order system, where the damping ratio ζ is between 0 and 1, a unit-step input results in a transfer function that, when transformed using the inverse Laplace method, reveals the output response. The output exhibits a damped sinusoidal oscillation, and the difference between the input and output is termed the error signal. This error signal also demonstrates damped oscillatory behavior. Eventually, as the system reaches a steady state, the error diminishes to zero.
If  ζ...
Relation between Mathematical Equations and Block Diagrams01:20

Relation between Mathematical Equations and Block Diagrams

In a spring-mass-damper system, the second-order differential equation describes the dynamic behavior of the system. When transformed into the Laplace domain under zero initial conditions, this equation can be effectively analyzed and manipulated. The transformation into the Laplace domain converts differential equations into algebraic equations, simplifying the process of isolating the output.
Elastic Strain Energy for Shearing Stresses01:20

Elastic Strain Energy for Shearing Stresses

As discussed in previous lessons, strain energy in a material is the energy stored when it is elastically deformed, a concept crucial in materials science and mechanical engineering. This energy results from the internal work done against the cohesive forces within the material. When a material undergoes shearing stress and corresponding shearing strain, the strain energy density, which is the energy stored per unit volume, is calculated. Within the elastic limit, where the stress is...
Circular Shaft - Stresses in Linear Range01:13

Circular Shaft - Stresses in Linear Range

Consider a scenario where a circular shaft is subject to torque that remains within the boundaries of Hooke's Law, avoiding any permanent deformation. So, the formula for shearing strain is revisited. This formula is multiplied by the modulus of rigidity, and then Hooke's Law for the shearing stress and strain is applied. As a result, the equation for shearing stress in a shaft can be derived.

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Related Experiment Videos

Nonequilibrium mode-coupling theory for uniformly sheared underdamped systems.

Koshiro Suzuki1, Hisao Hayakawa

  • 1Analysis Technology Development Center, Canon Inc., 30-2 Shimomaruko 3-chome, Tokyo 146-8501, Japan. suzuki.koshiro@canon.co.jp

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|February 16, 2013
PubMed
Summary

This study develops nonequilibrium mode-coupling theory (MCT) for underdamped systems, revealing significant yield stress relaxation and inertia effects not seen in overdamped systems.

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Area of Science:

  • Physics
  • Soft Matter Physics
  • Theoretical Physics

Background:

  • Nonequilibrium mode-coupling theory (MCT) is crucial for understanding complex systems.
  • Existing MCT models often focus on overdamped systems, limiting applicability to underdamped scenarios.
  • Bridging the gap between simulations and theory for underdamped systems remains a challenge.

Purpose of the Study:

  • To develop a nonequilibrium mode-coupling theory (MCT) for uniformly sheared underdamped systems.
  • To incorporate translational invariance and isothermal conditions within the theoretical framework.
  • To resolve existing contradictions in MCT for sheared systems.

Main Methods:

  • Starting from microscopic Sllod and Liouville equations.
  • Defining transient time correlators for translational invariance in sheared frames.
  • Implementing isothermal conditions via current fluctuation in dissipative coupling.

Main Results:

  • Developed a translationally invariant MCT equation for underdamped systems.
  • Observed pronounced yield stress relaxation due to growing current fluctuations in the alpha relaxation regime.
  • Identified an inertia effect in response to shear rate perturbations, absent in overdamped cases.

Conclusions:

  • The new MCT provides a more accurate description of underdamped sheared systems.
  • This work resolves contradictions between previous theoretical approaches (Fuchs-Cates and Chong-Kim).
  • The theory bridges the gap between molecular dynamics simulations and existing MCT models.