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Related Concept Videos

Characteristics of Fluids01:20

Characteristics of Fluids

When a force is applied parallel to the top surface of a solid, it resists the applied force due to the internal frictional forces between the layers of the solid known as shearing resistance. However, when the force is removed, the shearing forces restore the original shape of the solid. Other deformation forces also cause temporary changes in shape if the forces are not beyond a threshold magnitude. Solids tend to retain their shape, making the study of their rest and motion easier. Beyond...
Characteristics of Fluids01:31

Characteristics of Fluids

Fluids differ from solids primarily in their molecular structure and stress response. Solids have tightly packed molecules with strong intermolecular forces, maintaining their shape and resisting deformation. In contrast, fluids have molecules spaced farther apart with weaker forces, allowing them to flow and deform easily.
Fluids, which include both liquids and gases, are substances that deform continuously under shearing stress. For example, water and oil are liquids with molecules that can...
Newtonian Fluid: Problem Solving01:18

Newtonian Fluid: Problem Solving

Newtonian fluids exhibit a constant viscosity, meaning their shear stress and shear strain rate are directly proportional. This property ensures a predictable and stable response to applied forces, maintaining a linear relationship between force and flow. Examples include water, air, and light oils, consistently demonstrating this proportional behavior regardless of external conditions.
A velocity gradient forms within the fluid when a Newtonian fluid is placed between two parallel plates, with...
Equation of Continuity01:12

Equation of Continuity

Fluid motion is represented by either velocity vectors or streamlines. The volume of a fluid flowing past a given location through an area during a period of time is called the flow rate Q, or more precisely, the volume flow rate. Flow rate and velocity are related—for instance, a river has a greater flow rate if the velocity of the water in it is greater. However, the flow rate also depends on the size and shape of the river. The relationship between flow rate (Q) and average speed (v)...
The Principle of Superposition and the Gravitational Field01:17

The Principle of Superposition and the Gravitational Field

The principle of superposition applies to gravitational forces of objects that are sufficiently far apart. It states that the net gravitational force on a point object is the vector sum of the gravitational forces on it due to various objects. The principle helps calculate the force by listing the individual forces and then vectorially summing them up. However, it should be noted that the principle of superposition is not always apparent. In the presence of a second force, the first force could...
The Uncertainty Principle04:08

The Uncertainty Principle

Werner Heisenberg considered the limits of how accurately one can measure properties of an electron or other microscopic particles. He determined that there is a fundamental limit to how accurately one can measure both a particle’s position and its momentum simultaneously. The more accurate the measurement of the momentum of a particle is known, the less accurate the position at that time is known and vice versa. This is what is now called the Heisenberg uncertainty principle. He mathematically...

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An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
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Is there a "most perfect fluid" consistent with quantum field theory?

Thomas D Cohen1

  • 1Department of Physics, University of Maryland, College Park, Maryland 20742, USA.

Physical Review Letters
|August 7, 2007
PubMed
Summary

A conjecture proposed a universal lower bound for the ratio of shear viscosity to entropy density (eta/s) in fluids. This study demonstrates a counterexample in quantum chromodynamics (QCD), suggesting no such universal bound exists for metastable fluids.

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Area of Science:

  • High-energy physics
  • Fluid dynamics
  • Quantum field theory

Background:

  • A conjecture suggests a universal lower bound for the ratio of shear viscosity to entropy density (eta/s) for all fluids.
  • Theoretical counterexamples exist for nonrelativistic systems by increasing species number.
  • The study investigates if relativistic quantum field theory preserves this universal bound.

Purpose of the Study:

  • To determine if relativistic quantum field theory (QFT) imposes a universal lower bound on the shear viscosity to entropy density ratio (eta/s).
  • To explore the possibility of constructing a counterexample to the eta/s bound within a QFT framework.

Main Methods:

  • Analysis of a metastable gas of heavy mesons within a controlled regime of Quantum Chromodynamics (QCD).
  • Application of conservative assumptions to evaluate the system's properties within QFT.

Main Results:

  • A metastable gas of heavy mesons in QCD provides a realization of a theoretical counterexample to the eta/s bound.
  • This system is consistent with a well-defined underlying relativistic quantum field theory.

Conclusions:

  • Quantum field theory does not appear to impose a universal lower bound on the ratio of shear viscosity to entropy density (eta/s).
  • Metastable fluids, specifically heavy meson gases in QCD, can violate the conjectured eta/s bound.