Continuing Solutions of \(\displaystyle\dot{{{x}}}={\frac{{{t}^{{2}}{x}^{{5}}}}{{{1}+{x}^{{2}}+{x}^{{4}}}}}\) to entire number

Amya Horn

Amya Horn

Answered question

2022-03-27

Continuing Solutions of x˙=t2x51+x2+x4 to entire number line
can be continued to the whole real line.
I know that this ODE is seperable as follows
1+x2+x4x5dx=t2dt
Thus, giving the solution
14x412x2+ln(|x|)+C=13t3
However, forom here, it is not clear to me how any solution x(t) can be continued to the entire real number line.

Answer & Explanation

Aarlenlsi1

Aarlenlsi1

Beginner2022-03-28Added 10 answers

Explanation:
By comparing the degrees, the right side of the equation is linearly bounded in the x-direction, this can be made quantitative like
|x˙|t2|x||x(t)||x(0)|e|t|33.
At first this only holds on the domain where the solution x exists. But as this means that there can be no divergence to infinity at finite times, the domain can be extended without obstacle, so the maximal domain is the full real line.
horieblersee275

horieblersee275

Beginner2022-03-29Added 17 answers

Step 1
While Lutz's answer is the most succinct, the approach in the question is valid, albeit more work.
It is clear from Picard-Lindelöf that local solutions exist and are unique.
Note that x(t)=0 for all t is a solution. In particular, if x is a solution, and x(t)0 for some t, then x(t)0 for all t, and by continuity we see that if x is a solution defined on some interval I then exactly one of the following three cases holds: (i) x(t)=0 for all tI, (ii) x(t)>0 for all tI and (iii) x(t)<0 for all tI.
Step 2
Since f(x,t)=t2x51+x2+x4 is odd in x, we see that if x is a solution, then so is -x. Hence we can focus on Case (ii). All that needs to be done is to show that if there is a solution x(t)>0 for tI then it is defined on R (or rather, it can be extended to).
The function ϕ(x)=-14x4-12x2+logx is defined for t>0, smooth and ϕ(t)>0 for all t>0, hence has a smooth inverse.
Define y(t)=ϕ-1(ϕ(x(t0)+13(t3-t03)), note that y(t0)=x(t0) and ϕ(y(t))y(t)=t2, or y(t)=f(y(t),t), hence y(t)=x(t) for tI. Hence y is the extension we are looking for.

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