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Show that any nontrivial solution to $-u'' + q(x)u = 0$ has finitely many zeros
The Next CEO of Stack OverflowA solution $y$ of a Nth order homogenous linear ODE has infinite number of zeros on a closed interval. Prove the $y$ is identically $0$.Zero's of non trivial solution of an ODE.How can I determine how many solutions an Initial Value Problem has?Slight confusion on Lyapunov Stability of any solutionQuestion about theorem for reduction of order!If a corresponding homogeneous system of an inhomogeneous system has non-trivial solution, the inhomogeneous one has infinitely many solutions.How?Has $f'(x)=f(x+1/2)$ non-oscillating solutions?If $q(x)le 0$ on an interval $I$, then no non-trivial solution $y''+q(x)y=0$ an have two zeros on $I$.ODE with various initial conditionsShow that the solution of an IVP eventually leaves a compact set
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I am looking through an example and need some help to understand it.
For the problem $-u'' + q(x)u = 0$, where $0<x<1$, $q in mathcalC(0,1]$ and $x^2q(x) rightarrow q_0$ as $x rightarrow 0^+$, the goal is to show that any non-trivial solution only has finitely many zeros if $q_0 > -1/4$.
If $q_0 > -1/4$, then we can use Sturm's comparison theorem, and compare our equation with $-u'' - frac14x^2u = 0$, and the solution $sqrtx$. We see that $sqrtx$ has no zero in $(0,1]$, and since $q(x) > -1/4$ for sufficiently small $x$, we have that any non-trivial solution $u$ to $-u'' + q(x)u = 0$ can't have an accumulation of zeros at $x=0$. This part I understand.
Next, it says that it can also only have finitely many zeros in $(0,1]$, because otherwise the zeros would accumulate at some point $x_0$, and this would imply that $u(x_0) = u'(x_0)$ (which in turn implies that $u(x) equiv 0$).
The part that I don't quite understand is why an accumulation of zeros at $x_0$ implies that $u(x_0) = u'(x_0)$.
I had a thought that if we didn't have $u(x) equiv 0$, we would have a solution that kept oscillating for all future times around $x_0$ (if there were infinitely many zeros there) but I can't quite piece it together. Can such a solution not exist? Or does it have to do with something else entirely?
ordinary-differential-equations sturm-liouville
$endgroup$
add a comment |
$begingroup$
I am looking through an example and need some help to understand it.
For the problem $-u'' + q(x)u = 0$, where $0<x<1$, $q in mathcalC(0,1]$ and $x^2q(x) rightarrow q_0$ as $x rightarrow 0^+$, the goal is to show that any non-trivial solution only has finitely many zeros if $q_0 > -1/4$.
If $q_0 > -1/4$, then we can use Sturm's comparison theorem, and compare our equation with $-u'' - frac14x^2u = 0$, and the solution $sqrtx$. We see that $sqrtx$ has no zero in $(0,1]$, and since $q(x) > -1/4$ for sufficiently small $x$, we have that any non-trivial solution $u$ to $-u'' + q(x)u = 0$ can't have an accumulation of zeros at $x=0$. This part I understand.
Next, it says that it can also only have finitely many zeros in $(0,1]$, because otherwise the zeros would accumulate at some point $x_0$, and this would imply that $u(x_0) = u'(x_0)$ (which in turn implies that $u(x) equiv 0$).
The part that I don't quite understand is why an accumulation of zeros at $x_0$ implies that $u(x_0) = u'(x_0)$.
I had a thought that if we didn't have $u(x) equiv 0$, we would have a solution that kept oscillating for all future times around $x_0$ (if there were infinitely many zeros there) but I can't quite piece it together. Can such a solution not exist? Or does it have to do with something else entirely?
ordinary-differential-equations sturm-liouville
$endgroup$
1
$begingroup$
I think you missed part of that conclusion, it is that $u(x_0)=0$ as accumulation point and $u'(x_0)=0$ by the mean value theorem. As both are zero, one may shortly write $u(x_0)=u'(x_0)=0$.
$endgroup$
– LutzL
Mar 20 at 6:25
$begingroup$
Yes, it is clear to me now. Thank you. :)
$endgroup$
– RickS
Mar 21 at 10:22
add a comment |
$begingroup$
I am looking through an example and need some help to understand it.
For the problem $-u'' + q(x)u = 0$, where $0<x<1$, $q in mathcalC(0,1]$ and $x^2q(x) rightarrow q_0$ as $x rightarrow 0^+$, the goal is to show that any non-trivial solution only has finitely many zeros if $q_0 > -1/4$.
If $q_0 > -1/4$, then we can use Sturm's comparison theorem, and compare our equation with $-u'' - frac14x^2u = 0$, and the solution $sqrtx$. We see that $sqrtx$ has no zero in $(0,1]$, and since $q(x) > -1/4$ for sufficiently small $x$, we have that any non-trivial solution $u$ to $-u'' + q(x)u = 0$ can't have an accumulation of zeros at $x=0$. This part I understand.
Next, it says that it can also only have finitely many zeros in $(0,1]$, because otherwise the zeros would accumulate at some point $x_0$, and this would imply that $u(x_0) = u'(x_0)$ (which in turn implies that $u(x) equiv 0$).
The part that I don't quite understand is why an accumulation of zeros at $x_0$ implies that $u(x_0) = u'(x_0)$.
I had a thought that if we didn't have $u(x) equiv 0$, we would have a solution that kept oscillating for all future times around $x_0$ (if there were infinitely many zeros there) but I can't quite piece it together. Can such a solution not exist? Or does it have to do with something else entirely?
ordinary-differential-equations sturm-liouville
$endgroup$
I am looking through an example and need some help to understand it.
For the problem $-u'' + q(x)u = 0$, where $0<x<1$, $q in mathcalC(0,1]$ and $x^2q(x) rightarrow q_0$ as $x rightarrow 0^+$, the goal is to show that any non-trivial solution only has finitely many zeros if $q_0 > -1/4$.
If $q_0 > -1/4$, then we can use Sturm's comparison theorem, and compare our equation with $-u'' - frac14x^2u = 0$, and the solution $sqrtx$. We see that $sqrtx$ has no zero in $(0,1]$, and since $q(x) > -1/4$ for sufficiently small $x$, we have that any non-trivial solution $u$ to $-u'' + q(x)u = 0$ can't have an accumulation of zeros at $x=0$. This part I understand.
Next, it says that it can also only have finitely many zeros in $(0,1]$, because otherwise the zeros would accumulate at some point $x_0$, and this would imply that $u(x_0) = u'(x_0)$ (which in turn implies that $u(x) equiv 0$).
The part that I don't quite understand is why an accumulation of zeros at $x_0$ implies that $u(x_0) = u'(x_0)$.
I had a thought that if we didn't have $u(x) equiv 0$, we would have a solution that kept oscillating for all future times around $x_0$ (if there were infinitely many zeros there) but I can't quite piece it together. Can such a solution not exist? Or does it have to do with something else entirely?
ordinary-differential-equations sturm-liouville
ordinary-differential-equations sturm-liouville
asked Mar 19 at 22:17
RickSRickS
778
778
1
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I think you missed part of that conclusion, it is that $u(x_0)=0$ as accumulation point and $u'(x_0)=0$ by the mean value theorem. As both are zero, one may shortly write $u(x_0)=u'(x_0)=0$.
$endgroup$
– LutzL
Mar 20 at 6:25
$begingroup$
Yes, it is clear to me now. Thank you. :)
$endgroup$
– RickS
Mar 21 at 10:22
add a comment |
1
$begingroup$
I think you missed part of that conclusion, it is that $u(x_0)=0$ as accumulation point and $u'(x_0)=0$ by the mean value theorem. As both are zero, one may shortly write $u(x_0)=u'(x_0)=0$.
$endgroup$
– LutzL
Mar 20 at 6:25
$begingroup$
Yes, it is clear to me now. Thank you. :)
$endgroup$
– RickS
Mar 21 at 10:22
1
1
$begingroup$
I think you missed part of that conclusion, it is that $u(x_0)=0$ as accumulation point and $u'(x_0)=0$ by the mean value theorem. As both are zero, one may shortly write $u(x_0)=u'(x_0)=0$.
$endgroup$
– LutzL
Mar 20 at 6:25
$begingroup$
I think you missed part of that conclusion, it is that $u(x_0)=0$ as accumulation point and $u'(x_0)=0$ by the mean value theorem. As both are zero, one may shortly write $u(x_0)=u'(x_0)=0$.
$endgroup$
– LutzL
Mar 20 at 6:25
$begingroup$
Yes, it is clear to me now. Thank you. :)
$endgroup$
– RickS
Mar 21 at 10:22
$begingroup$
Yes, it is clear to me now. Thank you. :)
$endgroup$
– RickS
Mar 21 at 10:22
add a comment |
0
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I think you missed part of that conclusion, it is that $u(x_0)=0$ as accumulation point and $u'(x_0)=0$ by the mean value theorem. As both are zero, one may shortly write $u(x_0)=u'(x_0)=0$.
$endgroup$
– LutzL
Mar 20 at 6:25
$begingroup$
Yes, it is clear to me now. Thank you. :)
$endgroup$
– RickS
Mar 21 at 10:22