On Recent Advances of the 3D Euler Equations by Means of Examples (2024)

August 14, 2024

10:30AM - 11:30AM

Math Tower 154


Add to Calendar2024-08-14 10:30:002024-08-14 11:30:00On Recent Advances of the 3D Euler Equations by Means of Examples Edriss S. TitiUniversity of Cambridge Texas A&M University and Weizmann Institute of ScienceIn this talk we will use a basic example of shear flow to demonstrate some of the recent advances in the three-dimensional Euler equations. Specifically, this example was introduced by DiPerna and Majda to show that weak limit of classical solutions of Euler equations may, in some cases, fail to be a weak solution of Euler equations. We use this shear flow example to show the immediate loss of smoothness and ill-posedness of solutions of the 3D Euler equations, for initial data that do not belong to C 1,α. Moreover, we also show the existence of weak solutions for the 3D Euler equations with vorticity that is having a nontrivial density concentrated on non-smooth surface (vortex sheet). This is very different from what has been proven for the two-dimensional KelvinHelmholtz (Birkhoff-Rott) problem where a minimal regularity implies the real analyticity of the interface. Furthermore, we use this shear flow to provide explicit examples of non-regular solutions of the three-dimensional Euler equations that conserve the energy, an issue which is related to the Onsager conjecture. Eventually, we will discuss the recent remarkable work of De Lellis and Sz´ekelyhidi concerning the wild weak solutions of Euler equations and their non-uniqueness. In particular, we propose the following ruling out criterion for non-physical weak solutions of Euler equations: “In the absence of physical boundaries any weak solution of Euler equations which is not a vanishing viscosity limit of Leray-Hopf weak solutions of the Navier-Stokes equations should be ruled out”. We will use this shear flow, and other solutions of Euler equations with certain spatial symmetry, to provide nontrivial examples for the use of this ruling out criterion. If time allows we will also discuss (i) recent progress concerning the Onsager conjecture in bounded domains; (ii) the nonuniqueness of weak solutions to the 3D Navier-Stokes equations with Hyper-viscosity (−∆)θ , for θ < 5/4, demonstrating the sharpness of the J.-L. Lions result. Math Tower 154 OSU ASC Drupal 8ascwebservices@osu.eduAmerica/New_Yorkpublic

Date Range

Add to Calendar 2024-08-14 10:30:00 2024-08-14 11:30:00 On Recent Advances of the 3D Euler Equations by Means of Examples &nbsp;Edriss S. Titi&nbsp;University of Cambridge Texas A&amp;M University and Weizmann Institute of ScienceIn this talk we will use a basic example of shear flow to demonstrate some of the recent advances in the three-dimensional Euler equations. Specifically, this example was introduced by DiPerna and Majda to show that weak limit of classical solutions of Euler equations may, in some cases, fail to be a weak solution of Euler equations. We use this shear flow example to show the immediate loss of smoothness and ill-posedness of solutions of the 3D Euler equations, for initial data that do not belong to C 1,α. Moreover, we also show the existence of weak solutions for the 3D Euler equations with vorticity that is having a nontrivial density concentrated on non-smooth surface (vortex sheet). This is very different from what has been proven for the two-dimensional KelvinHelmholtz (Birkhoff-Rott) problem where a minimal regularity implies the real analyticity of the interface. Furthermore, we use this shear flow to provide explicit examples of non-regular solutions of the three-dimensional Euler equations that conserve the energy, an issue which is related to the Onsager conjecture. Eventually, we will discuss the recent remarkable work of De Lellis and Sz´ekelyhidi concerning the wild weak solutions of Euler equations and their non-uniqueness. In particular, we propose the following ruling out criterion for non-physical weak solutions of Euler equations: “In the absence of physical boundaries any weak solution of Euler equations which is not a vanishing viscosity limit of Leray-Hopf weak solutions of the Navier-Stokes equations should be ruled out”. We will use this shear flow, and other solutions of Euler equations with certain spatial symmetry, to provide nontrivial examples for the use of this ruling out criterion. If time allows we will also discuss (i) recent progress concerning the Onsager conjecture in bounded domains; (ii) the nonuniqueness of weak solutions to the 3D Navier-Stokes equations with Hyper-viscosity (−∆)θ , for θ &lt; 5/4, demonstrating the sharpness of the J.-L. Lions result. Math Tower 154 Department of Mathematics math@osu.edu America/New_York public

Edriss S. Titi

University of Cambridge Texas A&M University and Weizmann Institute of Science

In this talk we will use a basic example of shear flow to demonstrate some of the recent advances in the three-dimensional Euler equations. Specifically, this example was introduced by DiPerna and Majda to show that weak limit of classical solutions of Euler equations may, in some cases, fail to be a weak solution of Euler equations. We use this shear flow example to show the immediate loss of smoothness and ill-posedness of solutions of the 3D Euler equations, for initial data that do not belong to C 1,α. Moreover, we also show the existence of weak solutions for the 3D Euler equations with vorticity that is having a nontrivial density concentrated on non-smooth surface (vortex sheet). This is very different from what has been proven for the two-dimensional KelvinHelmholtz (Birkhoff-Rott) problem where a minimal regularity implies the real analyticity of the interface. Furthermore, we use this shear flow to provide explicit examples of non-regular solutions of the three-dimensional Euler equations that conserve the energy, an issue which is related to the Onsager conjecture. Eventually, we will discuss the recent remarkable work of De Lellis and Sz´ekelyhidi concerning the wild weak solutions of Euler equations and their non-uniqueness. In particular, we propose the following ruling out criterion for non-physical weak solutions of Euler equations: “In the absence of physical boundaries any weak solution of Euler equations which is not a vanishing viscosity limit of Leray-Hopf weak solutions of the Navier-Stokes equations should be ruled out”. We will use this shear flow, and other solutions of Euler equations with certain spatial symmetry, to provide nontrivial examples for the use of this ruling out criterion. If time allows we will also discuss (i) recent progress concerning the Onsager conjecture in bounded domains; (ii) the nonuniqueness of weak solutions to the 3D Navier-Stokes equations with Hyper-viscosity (−∆)θ , for θ < 5/4, demonstrating the sharpness of the J.-L. Lions result.

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On Recent Advances of the 3D Euler Equations by Means of Examples (2024)

FAQs

What is the application of the Euler equation of motion? ›

The Euler equations can be applied to incompressible and compressible flows. The incompressible Euler equations consist of Cauchy equations for conservation of mass and balance of momentum, together with the incompressibility condition that the flow velocity is a solenoidal field.

What is the significance of the Euler's equation? ›

Euler's equations are derived from the Navier-Stokes equations or from basic equations in continuum mechanics. Although Euler's equations consider a somewhat impossible physical situation of zero viscosity, they are useful for describing low-viscosity fluids like water or alcohols.

What is the difference between Navier Stokes and Euler equations? ›

The difference between them and the closely related Euler equations is that Navier–Stokes equations take viscosity into account while the Euler equations model only inviscid flow.

What is the primitive Euler equation? ›

The Euler equations

q=(ρρuE),f(q)=(ρuρu2+pu(E+p)).

What are the real life applications of Euler's equation? ›

Euler's formula, in engineering, is generally used for the analysis of complex numbers and waveforms. It helps in simplifying complex mathematical equations, in particular those involving trigonometric functions, and it's fundamental in the field of digital signal processing.

What is Euler's method used for in real life? ›

For example, Euler's method can be used to approximate the path of an object falling through a viscous fluid, the rate of a reaction over time, the flow of traffic on a busy road, to name a few.

Why is Euler's formula useful? ›

Euler's formula can also be used to provide alternate definitions to key functions such as the complex exponential function, trigonometric functions such as sine, cosine and tangent, and their hyperbolic counterparts. It can also be used to establish the relationship between some of these functions as well.

What is the use of Euler's number in real life? ›

It frequently appears in problems dealing with exponential growth or decay, where the rate of growth is proportionate to the existing population. In finance, e is also used in calculations of compound interest, where wealth grows at a set rate over time.

What does Euler's method tell you? ›

Euler's Method, is just another technique used to analyze a Differential Equation, which uses the idea of local linearity or linear approximation, where we use small tangent lines over a short distance to approximate the solution to an initial-value problem.

What does Navier-Stokes tell us? ›

The Navier–Stokes equations can be very useful in applied physics. Primarily, they help to describe the mechanics of various engineering and scientific phenomena. They could be applied to model ocean currents, weather, air flow around wings, and the flow of water in pipes.

What is the Euler's equation for fluid dynamics? ›

This states that the acceleration (rate of change of velocity) of a fluid particle is directly proportional to the net forces acting on it, including pressure force and gravitational force. Here F n e t = − ∇ p + ρ g → , representing the net force per unit volume on a fluid particle.

Is Navier-Stokes Lagrangian or Eulerian? ›

Lagrangian Navier-Stokes is written following a fluid particle as it moves, as opposed to Eulerian form which tracks the variables at fixed locations in space as the flow moves through them.

What is the most beautiful theorem in math? ›

A poll of readers conducted by The Mathematical Intelligencer in 1990 named Euler's identity as the "most beautiful theorem in mathematics".

What is the famous Euler's equation? ›

Euler's formula, e i θ = cos ⁡ ( θ ) + i sin ⁡ ( θ ) , and the special case when θ = π is unequivocally beautiful. Since cos ⁡ ( π ) = − 1 and sin ⁡ ( π ) = 0 , we have e i π = − 1 ⟺ e i π + 1 = 0 , called Euler's identity, and widely considered the most beautiful equation in mathematics.

Does Euler's identity prove God? ›

The Euler's Identity proves only that e to (i x pi) is equal to minus 1. If this is God, fine, it also proves that God has a huge imaginary component that applies to Him exponentially. Since I've always thought God to be imaginary, this proof is good enough for me. God exists, but He is imaginary.

What is the application of Euler function? ›

It is commonly used in encryption algorithms, primality testing, and solving modular arithmetic problems. Euler's totient function comes into play whenever there is a need to analyze the properties of prime numbers or determine the number of relatively prime integers to a given number.

What is the application of Euler's theory? ›

Applications of Euler's Theorem

RSA utilizes Euler's theorem in the process of encryption and decryption. In RSA, the public and private keys are generated in such a way that they are inverses of each other modulo φ(n), where n is the product of two large prime numbers.

What is Euler's theorem and its application? ›

Euler's theorem lays the groundwork for understanding various aspects of modular arithmetic, which has applications in cryptography, computer science, and various other fields. It states that if a and n are coprime (i.e., their greatest common divisor is 1), then (−1) ≡ 1(mod)a (n−1) ≡1(modn).

What is the application of Euler's model law? ›

The Euler-Euler model has no limitations on particle numbers being simulated and it can be applied to model dense phase gas solid flow, such as bypass pneumatic conveying. There are three types of Euler-Euler models: the Volume of Fluid (VOF) model, the mixture model and the Eulerian model, as summarized in Table 2.

References

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