Hey guys, take a look at my work for a stationary integral?

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Homework Help Overview

The problem involves finding a stationary path for an integral defined between points O=(0,0) and P=(0,4). The integral in question is expressed as the square root of a function involving x and the derivative of y with respect to x.

Discussion Character

  • Exploratory, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the application of calculus of variations, attempting to derive necessary conditions for stationarity. There are attempts to differentiate expressions involving y and its derivatives, with some participants questioning the correctness of the derivatives and the presence of terms like y''.

Discussion Status

The discussion is ongoing, with participants providing feedback on each other's mathematical expressions and reasoning. Some have expressed uncertainty about the implications of their findings, particularly regarding the complexity of the resulting equations. There is a recognition that the problem may lead to a nonlinear ordinary differential equation, which raises concerns about the path forward.

Contextual Notes

Participants note the challenge of dealing with a nonlinear ordinary differential equation and express apprehension about whether their current approach will yield a solution to the original problem.

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Homework Statement



Path between O=(0,0) and P=(0,4) for which the integral

int. O to P (x (1-y'^2))^(1/2) dx

becomes stationary.


Homework Equations



http://en.wikipedia.org/wiki/Calculus_of_variations#Example

The Attempt at a Solution



Okay guys,

so mimicking the example from wiki but with L= (x)^1/2 (1-y'^2)^1/2

dL/dy=0 and dL/dy'= -(x)^1/2 y' / (1-y'^2)^1/2 and then d/dx dL/df' = - y'/[(2x^1/2)(1-y'^2)^1/2]

and since d/dx dL/df' =0 this implies y'=0 and we integrate to get y=c, adhering to boundary conditions y must equal 0... was that the correct way sorry for not writing in latex if I must I will redo the post
 
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Kidphysics said:
dL/dy'= -(x)^1/2 y' / (1-y'^2)^1/2 and then d/dx dL/df' = - y'/[(2x^1/2)(1-y'^2)^1/2]
That last expression looks too simple. There should be a y" in there, and two different powers of x. Remember it's not a partial derivative this time.
 
haruspex said:
That last expression looks too simple. There should be a y" in there, and two different powers of x. Remember it's not a partial derivative this time.

ahhhh you are correct! y is a function of x..
 
well.. I used the product rule and the chain rule and now I am looking at an unbelievable

2 x^1/2 y'^2 y'' - 1/2 x^-1/2 y' - x^1/2 y'' + 1/2 x^-1/2 y'^3 =0 .

I believe I took the derivative correctly this time but now I am lost as what to do with this..
 
haruspex said:
That last expression looks too simple. There should be a y" in there, and two different powers of x. Remember it's not a partial derivative this time.

well.. I used the product rule and the chain rule and now I am looking at an unbelievable

2 x^1/2 y'^2 y'' - 1/2 x^-1/2 y' - x^1/2 y'' + 1/2 x^-1/2 y'^3 =0 .

I believe I took the derivative correctly this time but now I am lost as what to do with this.
 
Allow me to put that in LaTex:

[tex]2 x^{1/2} y'^2 y'' - (1/2)x^{-1/2} y' - x^{1/2} y'' + (1/2) x^{-1/2} y'^3 =0 [/tex]
Simplifying:
[tex]4 x y'^2 y'' - y' - 2x y'' + y'^3 =0[/tex]
But that's not quite what I get. Writing K = (1-y'2)1/2:
L = x1/2K
∂K/∂y' = -y'/K
∂L/∂y' = -x1/2y'/K
[tex]0 = -\frac{d(∂L/∂y')}{dx} = \frac{x^{-1/2}y'}{2K} + \frac{x^{1/2}y''}{K} - \frac{x^{1/2}y'\frac{∂K}{∂y'}y''}{K^2}[/tex]
[tex]0 = y'+ 2xy'' - 2\frac{xy'\frac{∂K}{∂y'}y''}{K}[/tex]
[tex]0 = y'+ 2xy'' + 2\frac{xy'^2y''}{K^2}[/tex]
[tex]0 = (y'+ 2xy'')(1-y'^2) + 2xy'^2y''[/tex]
[tex]0 = y'+ 2xy'' - y'^3[/tex]
Is that right or did I get sign wrong somewhere?
 
haruspex said:
Allow me to put that in LaTex:

[tex]2 x^{1/2} y'^2 y'' - (1/2)x^{-1/2} y' - x^{1/2} y'' + (1/2) x^{-1/2} y'^3 =0 [/tex]
Simplifying:
[tex]4 x y'^2 y'' - y' - 2x y'' + y'^3 =0[/tex]
But that's not quite what I get. Writing K = (1-y'2)1/2:
L = x1/2K
∂K/∂y' = -y'/K
∂L/∂y' = -x1/2y'/K
[tex]0 = -\frac{d(∂L/∂y')}{dx} = \frac{x^{-1/2}y'}{2K} + \frac{x^{1/2}y''}{K} - \frac{x^{1/2}y'\frac{∂K}{∂y'}y''}{K^2}[/tex]
[tex]0 = y'+ 2xy'' - 2\frac{xy'\frac{∂K}{∂y'}y''}{K}[/tex]
[tex]0 = y'+ 2xy'' + 2\frac{xy'^2y''}{K^2}[/tex]
[tex]0 = (y'+ 2xy'')(1-y'^2) + 2xy'^2y''[/tex]
[tex]0 = y'+ 2xy'' - y'^3[/tex]
Is that right or did I get sign wrong somewhere?

hey thanks, jumped out of bed to respond.. I'm sure you have the math correct but I can't see how this helps us get a solution the the original problem. At this step we have a nonlinear ode so I'm a little frightened we are on the wrong track? Thank you for helping thus far
 
haruspex said:
[tex]0 = y'+ 2xy'' - y'^3[/tex]
It's not hard from there. There are no y terms, so it's first order, and you can get it into the form f(x) = g(t)t' where t = y', so then it's just an integration to get an equation relating x to y'.
 

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