Two Variable PDE in Open Domain Plane

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Discussion Overview

The discussion revolves around a two-variable partial differential equation (PDE) in an open domain of the plane, exploring its structure and potential solutions. Participants examine various transformations and methods, including separation of variables and the method of characteristics, while also discussing the context from which the equation arises.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant presents the PDE in the form of a ratio involving functions U and V, suggesting a potential separation of variables approach.
  • Another participant questions whether a specific transformation simplifies the problem, noting that Mathematica indicates an indeterminate form due to more dependent variables than equations.
  • A different participant reformulates the equation using logarithmic derivatives and proposes a guess for the ratio of U to V, leading to a new equation that remains unsolved.
  • Another participant provides a similar reformulation and suggests that the resulting equation can be solved using characteristics, presenting a solution involving an arbitrary constant.
  • One participant expresses a desire to learn more about differential equations and mentions their current study of differential geometry.
  • Another participant shares their self-taught experience with the method of characteristics in relation to their research problems.
  • A participant explains the origin of the equation, linking it to vector fields on surfaces and geodesics in differential geometry, suggesting that the solution indicates certain hyperbolas can be geodesics.

Areas of Agreement / Disagreement

Participants express various approaches and interpretations of the PDE, with no consensus on a definitive solution or method. Multiple competing views and methods are presented, indicating an ongoing exploration of the topic.

Contextual Notes

The discussion includes unresolved mathematical steps and assumptions regarding the nature of the functions U and V, as well as the implications of the derived equations in the context of differential geometry.

Who May Find This Useful

Readers interested in partial differential equations, mathematical methods in physics, and applications in differential geometry may find this discussion relevant.

lavinia
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In an open domain in the plane

(xU_{x}-yU_{y}-U)/U =

(xV_{x} - y V_{y}+V)/V
 
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I'd like to know the answer myself. Does \frac{xU_x}{U}-\frac{xV_x}{V}=\frac{yU_y}{U}-\frac{yV_y}{V} make it any easier? I've only dabbled in PDEs myself, but that seems like a separation of variables problem, when rephrased like that.

EDIT: Mathematica gives an error saying the answer is indeterminate, because there are more dependent variables than equations.
 
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TylerH said:
I'd like to know the answer myself. Does \frac{xU_x}{U}-\frac{xV_x}{V}=\frac{yU_y}{U}-\frac{yV_y}{V} make it any easier? I've only dabbled in PDEs myself, but that seems like a separation of variables problem, when rephrased like that.

EDIT: Mathematica gives an error saying the answer is indeterminate, because there are more dependent variables than equations.

U = x V = K/x sort of works but doesn't allow the origin or the y axis.
Also the answer is a little trivial.
 
So you have:
x d/dx ln (U) -y d/dy ln(U) -1 = xd/dx ln (V) -y d/dy ln(V) +1
x d/dx (ln(U/V))=y d/dy (ln(U/V))+2

Now make a guess of a function of the type U/V = exp(F(x,y))

to get:
x d/dx F = y d/dy F +2

so you have x d/dx F -y d/dy F =2

d/dx (xF) - d/dy (yF) = 2

Don't see how to solve this, though.

p.s the derivatives above are partial btw.
 
lavinia said:
In an open domain in the plane

(xU_{x}-yU_{y}-U)/U =

(xV_{x} - y V_{y}+V)/V

I would rewrite this as

x \partial_x (\log U) - y \partial_y (\log U) - 1 = x \partial_x (\log V) - y \partial_y (\log V) + 1

or

x \partial_x (\log U - \log V) - y \partial_y (\log U - \log V) = 2

Define some function e^f = U/V and you have

x \partial_x f - y \partial_y f = 2

which should be easy to solve by characteristics. Mathematica gives

f = 2 \log x + C x y

for arbitrary C. Then U and V can be any functions satisfying

\frac{U}{V} = x^2 e^{C x y}
 
Thanks Ben

What approach would you recommend to learning more about differential equations? Right now i am learning differential geometry.
 
I don't know, I taught myself the method of characteristics when I started running across problems in my research that needed it.
 
Sometime I wonder why I even bother answering. :-/
 
I thank you for this solution and feel that I should explain where this equation came from.

To learn some differential geometry I posed the question of what vector fields on a surface can be tangent to geodesics for some Riemannian metric. Computation led to the condition that a unit length vector field V is tangent to geodesics if its Lie bracket with iV, the unit vector field orthogonal to it, is a multiple of iV (and that this multiple satisfies a differential equation along the geodesic that relates it to the Gauss curvature of the metric).

For the vector field xd/dx - yd/dy in a neighborhood of the origin in the plane, one gets the differential equation in this post. I think your solution shows that the field of hyperbolas y = k/x can be geodesics and that iV can be chosen to be x^{2}d/dx + e^{-xy}d/dy.

So it seems that a vector field of index -1 around a singularity can be a geodesic flow.

I think the Gauss curvature is -1 for this example but I haven't yet done the ugly calculation.
 
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