Bachelorarbeit, 2010
35 Seiten, Note: 1,0
1. Introduction
2. Preliminaries
2.1. The Transport Theorem
2.2. Governing equations of fluid dynamics
2.3. Concepts of a solution
3. Analysis of the classical case
3.1. The classical Landau solution
3.2. Characterisation and approximation of solutions by the Landau solution
4. Analysis of the modified Landau solution
4.1. The critical Landau solution
4.2. The supercritical Landau solution
4.3. Summary and outlook
This thesis examines the properties of the Landau solution to the steady Navier-Stokes equations, focusing on the derivation, mathematical characterization, and the analysis of singular behaviors when moving from classical to critical and supercritical cases.
3.1 The classical Landau solution
Theorem 3.1.1. Let d ∈ (−1, 1). Then on R³\{0} a smooth solution (u, p) to the Navier-Stokes system (2.21) which is symmetric, but does not rotate about the x3-axis and fulfils the homogeneity conditions u(x)= 1/|x| u(x/|x|) and p(x)= 1/|x|² p(x/|x|) is given by (1.1). Such a solution is called a Landau solution. Furthermore, every smooth solution satisfying these conditions is a Landau solution.
Rather than checking all the conditions, we will derive the solution from the scratch to have a better insight in the physical meanings of the respective terms, which will help us understanding the more general situation later.
The main idea of our attempt to find a solution to the Navier-Stokes system is, that we reduce the problem to a solvable ordinary differential equation in only one variable. Even though the axisymmetry of the system might suggest cylindrical coordinates, it turns out that using spherical coordinates yields the fastest approach towards this, for then we can make use of our knowledge about the radial dependence of our solution. The proof provided here is due to [3] and [19].
Proof. Since the Navier-Stokes flow is assumed to be stationary and has, if one assumes in advance no rotation of the fluid around its axis of symmetry, only two degrees of freedom, the continuity equation is identically fulfilled by finding a stream function ψ as introduced in [3], such that the velocity components in spherical coordinates are described by u(r) = 1/(r² sin θ) ∂ψ/∂θ, u(θ) = − 1/(r sin θ) ∂ψ/∂r, u(φ) = 0.
1. Introduction: Presents the historical context of Lev D. Landau's 1944 solution to the stationary Navier-Stokes equations and introduces the mathematical framework and notation used throughout the paper.
2. Preliminaries: Establishes the fundamental fluid dynamics background, including the Transport Theorem, governing equations of mass and momentum conservation, and formal definitions of solution concepts.
3. Analysis of the classical case: Derives the classical Landau solution and provides a rigorous analysis of its properties, including the physical interpretation of the Landau parameter and its relation to fluid force.
4. Analysis of the modified Landau solution: Investigates the behavior of Landau solutions beyond the classical case, specifically focusing on critical and supercritical solutions that exhibit singular behavior at the origin or along a cone.
Navier-Stokes equations, Landau solution, fluid dynamics, spherical coordinates, stationary flow, axisymmetry, stream function, distributional solutions, critical Landau solution, supercritical Landau solution, momentum flux, continuity equation, singularity analysis.
The work focuses on the mathematical analysis of the Landau solution, which is a specific exact solution to the stationary Navier-Stokes equations representing a fluid flow driven by a point force.
The thesis covers the derivation of the Landau solution, the classification of classical versus singular (modified) solutions, and the physical interpretation of these flows in the context of fluid jets.
The primary objective is to determine if and how Landau solutions, particularly modified versions, can be extended to the whole space R³ and whether they provide a valid physical interpretation for fluid flow problems.
The author employs analytical methods from fluid dynamics, including the use of stream functions in spherical coordinates, distribution theory, and the study of ordinary differential equations derived from the Navier-Stokes system.
The main body systematically derives the classical Landau solution, analyzes its properties, and extends the investigation to critical and supercritical regimes to test the limits of these mathematical models.
Key terms include Navier-Stokes equations, Landau solution, axisymmetry, fluid dynamics, distributional solutions, and point singularities.
The Landau parameter is uniquely related to the force at the origin; a higher magnitude of the parameter corresponds to a stronger, faster, and narrower fluid stream.
The critical Landau solution exhibits behavior where streamlines tend toward the origin or a critical half-line, and calculations of the divergence show that the flow acts as a sink, complicating the physical interpretation in the whole space.
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