Second-Order Nonlinear Differential Equation

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SUMMARY

The discussion centers on solving the second-order nonlinear differential equation defined by \( y''(t)=-\frac{y(t)}{||y(t)||^3} \) with initial conditions \( y(0)= \begin{pmatrix} 1\\0 \end{pmatrix} \) and \( y'(0)= \begin{pmatrix} 0\\1 \end{pmatrix} \). Participants confirm that the solution exists and resembles the motion of an object under Newtonian gravity, leading to a conic section solution. The general solution is expressed as \( y(t)=r(t)(\cos\theta(t), \sin\theta(t)) \) with \( r(t)=\frac{b^2}{a-c\cos\theta(t)} \), ultimately simplifying to the unit circle \( y(t) = (\cos t, \sin t) \).

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  • Familiarity with Newtonian gravity concepts
  • Knowledge of conic sections and their properties
  • Basic skills in solving differential equations
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sav26
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Hi there can someone please help me with this differential equation, I'm having trouble solving it
$$
\begin{cases}

y''(t)=-\frac{y(t)}{||y(t)||^3} \ , \forall t >0
\\
y(0)= \Big(\begin{matrix} 1\\0\end{matrix} \Big) \
\text{and}
\
y'(0)= \Big(\begin{matrix} 0\\1\end{matrix} \Big)\end{cases}
\\

y(t) \in \mathbb{R}^2 \ \forall t
$$

Thanks in advance ^^
 
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Non-linear differential equations are, in general, extremely difficult and most simply do not have solutions in terms of elementary functions. Do you have any reason to believe this does or will a numerical solution suffice?
 
it must have solutions yes, it's in my homework and the following question requires these solutions
 
If I can see and remember correctly, this equation is similar than equation of motion of an object under Newtonian gravity. Thus the solution indeed exists, and in general the shape of the solution \( y(x) \) can be derived, but the time depense of coordinates \( (x(t), y(t)) \) can be impossible to write down. However, everything is easier in circular motion... :unsure:
 
Theia said:
If I can see and remember correctly, this equation is similar than equation of motion of an object under Newtonian gravity. Thus the solution indeed exists, and in general the shape of the solution \( y(x) \) can be derived, but the time depense of coordinates \( (x(t), y(t)) \) can be impossible to write down. However, everything is easier in circular motion...
Yeah, it is indeed the motion of an object in a field of central gravity.
So the solution is a conic section (ellipse, hyperbola, or parabola) with the origin as a focal point.
That is, the general solution of the differential equation is
$$y(t)=r(t)(\cos\theta(t), \sin\theta(t))$$
with $r(t)=\frac{b^2}{a-c\cos\theta(t)}$ and $r(t)^2 \theta'(t) = \text{constant}$.

Since every constant is $0$ or $1$, we can see by inspection that the solution is the unit circle.
That is
$$y(t) = (\cos t, \sin t).$$
Things are indeed easier in circular motion. :geek:
 
Last edited:

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