Non-linear second order from calculus of variation I can't solve

jackmell
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Hi,

I derived the equation:

[tex]1+(y')^2-y y''-2y\left(1+(y')^2\right)^{3/2}=0[/tex]

Letting [itex]y'=p[/itex] and [itex]y''=p\frac{dp}{dy}[/itex], I obtain:

[tex]\frac{dp}{dy}=\frac{1+p^2-2y(1+p^2)^{3/2}}{yp}[/tex]

I believe it's tractable in p because Mathematica gives a relatively simple answer:

[tex]p=\begin{cases}\frac{i \sqrt{-y^2+y^4-4 y^2 C[1]+4 C[1]^2}}{y^2-2 C[1]}\\<br /> \\<br /> -\frac{i \sqrt{-y^2+y^4-4 y^2 C[1]+4 C[1]^2}}{y^2-2 C[1]}<br /> \end{cases}[/tex]

I don't see how to get to that answer and I was wondering if someone here could help me with this.

Thanks,
Jack
 
on Phys.org
What does 'C[1]' represent?
 
SteamKing said:
What does 'C[1]' represent?

I should have changed that to just c. It's a constant:

[tex]p=\begin{cases}\frac{i \sqrt{-y^2+y^4-4 y^2 c+4 c^2}}{y^2-2 c}\\<br /> \\<br /> -\frac{i \sqrt{-y^2+y^4-4 y^2 c+4 c^2}}{y^2-2 c}<br /> \end{cases}[/tex]
 
Try the substitution

$$ w = \frac{\sqrt{1+p^2}}{y}.$$

You should find that

$$ \frac{dw}{dy} = -2y w^2,$$

which is separable.
 
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Hi !

A laborious method below :
 

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You guys are just shear art in here. [itex]\frac{dw}{dy}=-2w^2y[/itex] was tough for me to go through but I got it. Still working through Jacquelin's. I'm sure it's correct though. :)
 
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