I'm trying to change this sturm liouville equation into a boundary value problem. To no avail I cannot get it work. Can anyone help me out <3
with \(x = e^t\)
.
what does \(.\) mean
What did you try?
a bunch of scribbles getting no where I AM LOST
this is fked i swear i should ahve done operating systems
with x = e^t i should get to this https://gyazo.com/2405ad6a1ffabe622aa8c8d0939c65c0
but i am not getting there i am going in circles
i am getting like a humongous bunch of eqns
please try this substitution: \(\huge y=kx^s\)
i need this x = e^t
You shoulda done linear algebra bb
sry u don't know the chain rule I can't help you.
so help me with chain rule
I'm afraid this is beyond my current level, but if you want to learn about chain rules, you can go here: https://www.khanacademy.org/math/differential-calculus/taking-derivatives/chain_rule/v/chain-rule-introduction Khan Academy always provides free, detailed tutorials on these things. c:
getting to that thing you posted is not that hard. forget about sturm-louiville for a bit, that's the bit that's throwing me. i don't know what that reference means in the problem. this is a euler-caucy 2nd order linear DE, and you using the [much better, IMHO] change of independent variable substitution, \(x=e^t\), to solve ot this means \(xy' = Y'\), and \(x^2y'' = Y'' - Y'\) which you sub straight into your DE now in terms of independent variable t.[i presume your uppercase Y signifies that we are now working with our new independent varable t so i gave followed that convention.] so your DE in x becomes in t : \(Y'' - Y' + Y'+ \lambda Y = 0\) or \(Y'' + \lambda Y = 0\) which is what you want. to change the boundary values, again using \(x = e^t\) we have \(y(1)\) = 0, so \( Y(0) = 0\) as \(1 = e^0\), and \(y'(e) = Y'(1) = 0\). as for eigen stuff, i assume you are now going to create a system?
and if you can wait, someone like @SithsAndGiggles or @freckles is well worth waiting for.....
Borrowing from @IrishBoy123's comment, a change of variables \(x=e^t\), \(y(x)=Y(t)\) yields the linear ODE, \[Y''+\lambda Y=0~~\implies~~Y=C_1\cos(\sqrt\lambda t)+C_2\sin(\sqrt\lambda t)\]which is equivalent to \[y=C_1\cos(\sqrt\lambda \ln x)+C_2\sin(\sqrt\lambda \ln x)\]With the given boundary conditions, you get the following system: \[\begin{cases}C_1\cos0+C_2\sin0=0\\[1ex] -C_1\dfrac{\sqrt\lambda}{e}\sin(\sqrt \lambda)+C_2\dfrac{\sqrt\lambda}{e}\cos(\sqrt\lambda)=0\end{cases}\implies\begin{cases}C_1=0\\[1ex]C_2\cos(\sqrt\lambda)=0\end{cases}\]You want a nontrivial solution, so you require that \(C_2\neq0\). It should be easy to find the eigenvalues now.
Finding the eigenfunctions is easy enough once you determine \(\lambda\), so you would have \(y=\sin(\sqrt\lambda\ln x)\).
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