Fundamental solutions of the stokes equation.

In summary, to derive the stresslet and rotlet for the Stokes equations, one must expand the function Gik(x) as a Taylor series around the point x-0 and then plug it into the equation for ui. This can be done at both A/2 and -A/2, and the two solutions can then be added to obtain the final result of ui = 0. The mix of notation may be confusing, but by keeping in mind the point of expansion and the derivatives evaluated at that point, the problem can be solved.
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Homework Statement


Hi, I going through my class notes for a fluids class, specifically fundamental solutions of the Stokes equations. To derive the stresslet and rotlet involves solving the following

ui = (1/8*pi*μ)*(∂Gik/∂xj)*Fk*Aj

Gik(x) = δij*(1/r)+(xixj/r3)

We looked at it in a lecture (skipping all the "easy parts"! of course) and I am trying to fill in the gaps. The first step is to taylor expand it at A/2 wit |A/2| << |x|.

This should give ui(x) = (1/8*pi*μ)*(Gik(x-0)Fk + (Ai/2)*∂/∂xj(Gik)(x - 0)*Fk + ... (Mix of vector and suffix notation here very confusing)

Then do the same at -A/2 (with -F) and add the solutions

Homework Equations



Taylor series: f(a) + f'(a)*(x-a) + (f''(a)/2!)*(x-a)2 + ...


The Attempt at a Solution



My problem is the mix of notation, I am not sure how to apply the taylor series here. Any help appreciated.
 
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  • #2
Since Taylor's theorem is a local expansion, you can expand the function Gik(x) around the point x-0. To do this, start by expanding Gik(x) as a Taylor series around the point x-0. Since Gik(x) is a function of two variables (x and j) we need to differentiate with respect to both variables. We also need to keep in mind that the derivatives are evaluated at the point x-0, so for example the second derivative with respect to x is ∂2Gik/∂x2(x-0). The Taylor series can then be written as: Gik(x) = Gik(x-0) + (Ai/2)*∂Gik/∂xj(x-0) + (Ai/2)2*∂2Gik/∂xj2(x-0) + ...Plugging this into the equation for ui gives: ui = (1/8*pi*μ)*(Gik(x-0)Fk + (Ai/2)*∂Gik/∂xj(x-0)*Fk + (Ai/2)2*∂2Gik/∂xj2(x-0)*Fk + ... )Then do the same at -A/2 (with -F): ui = (1/8*pi*μ)*(-Gik(x-0)Fk - (Ai/2)*∂Gik/∂xj(x-0)*Fk - (Ai/2)2*∂2Gik/∂xj2(x-0)*Fk + ... )Adding the two solutions gives the final result: ui = (1/8*pi*μ)*[Gik(x-0)(Fk - Fk) + (Ai/2)*∂Gik/∂xj(x-0)*(Fk - Fk) + (Ai/2)2*∂2Gik/∂xj2(x-0)*(Fk - Fk) + ... ]
 

1. What is the Stokes equation?

The Stokes equation is a mathematical model that describes the motion of a viscous fluid under the influence of an external force, such as gravity or applied pressure. It takes into account the effects of both inertia and viscosity on the fluid's behavior.

2. What are fundamental solutions of the Stokes equation?

Fundamental solutions of the Stokes equation are exact solutions that satisfy the equation and represent the simplest form of fluid motion. They are typically used as building blocks to construct more complex solutions for practical problems.

3. What is the significance of fundamental solutions in fluid mechanics?

Fundamental solutions are important in fluid mechanics because they provide a fundamental understanding of the underlying physics and behavior of fluids. They also serve as a starting point for developing more sophisticated models and simulations for real-world applications.

4. How are fundamental solutions of the Stokes equation derived?

Fundamental solutions of the Stokes equation are derived by solving the equation with specific boundary and initial conditions. This involves using mathematical techniques, such as separation of variables and Fourier series, to find exact solutions that satisfy the equation and boundary conditions.

5. Can fundamental solutions be applied to all types of fluid flow?

No, fundamental solutions of the Stokes equation are only applicable to flows that are very slow and have low Reynolds numbers, meaning the effects of inertia are negligible compared to viscosity. They are not applicable to turbulent flows or flows with high Reynolds numbers.

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