Nonlinear equation analysis withe epsilon value [closed]












-1












$begingroup$


Consider the nonlinear equation
$$frac{d^2x}{dt^2}+epsilonsin(x)=0,~~epsilon ll 1\
x(0)=0,~~dot{x}(0)=1$$



and find...

A. The value of $x_0$ as $epsilon$ goes to $0$

B. The first order term $x_1$ and the second order term $x_2$

C. Plot $x(t)$ for $x_0$, $x_1$, and $x_2$

D. Assemble the solution $x=x_0(t)+epsilon x_1(t)+epsilon^2 x_2(t)$. Plot $x(t)=x_0(t)$, $x=x_0(t)+epsilon x_1(t)$ and $x+x_0(t)+epsilon x_1(t)+epsilon^2 x_2(t)$ on the same graph.



So the thought is that you can expand the sine function around $x=x_0$ to obtain the equations you need. Then, using Laplacian transforms, $x_1 and x_2$ are solvable.










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$endgroup$



closed as off-topic by MisterRiemann, the_candyman, Davide Giraudo, amWhy, KReiser Dec 8 '18 at 0:22


This question appears to be off-topic. The users who voted to close gave this specific reason:


  • "This question is missing context or other details: Please provide additional context, which ideally explains why the question is relevant to you and our community. Some forms of context include: background and motivation, relevant definitions, source, possible strategies, your current progress, why the question is interesting or important, etc." – MisterRiemann, Davide Giraudo, amWhy, KReiser

If this question can be reworded to fit the rules in the help center, please edit the question.













  • $begingroup$
    What is $x_0, x_1$ and $x_2$? Please, provide more details. Most importantly, add also your efforts. Otherwise, I feel that this question will be closed soon and you won't get any answer.
    $endgroup$
    – the_candyman
    Dec 7 '18 at 18:14










  • $begingroup$
    Where did you find this, or what prompted you to conceive it? It it essential that ε be small? And is there some slick answer? I would say it's not massively different from SHM, as when x gets to the domain in which sine levels-off, it will still be follwing a downward-curving parabola.
    $endgroup$
    – AmbretteOrrisey
    Dec 7 '18 at 18:38












  • $begingroup$
    Whoops, did not mean to post. I simply wanted to save for later. Regardless, I updated with more information and direction that I am headed.
    $endgroup$
    – Pascal
    Dec 7 '18 at 20:12






  • 2




    $begingroup$
    @Pascal -- I've done that! It's easy, isn't it, when you're using the fields here as your personal equation-editor ... but who would be so delinquent as to do a thing like that!!? ¶ Whhoops! I've just said ... I've done it!!
    $endgroup$
    – AmbretteOrrisey
    Dec 7 '18 at 20:48


















-1












$begingroup$


Consider the nonlinear equation
$$frac{d^2x}{dt^2}+epsilonsin(x)=0,~~epsilon ll 1\
x(0)=0,~~dot{x}(0)=1$$



and find...

A. The value of $x_0$ as $epsilon$ goes to $0$

B. The first order term $x_1$ and the second order term $x_2$

C. Plot $x(t)$ for $x_0$, $x_1$, and $x_2$

D. Assemble the solution $x=x_0(t)+epsilon x_1(t)+epsilon^2 x_2(t)$. Plot $x(t)=x_0(t)$, $x=x_0(t)+epsilon x_1(t)$ and $x+x_0(t)+epsilon x_1(t)+epsilon^2 x_2(t)$ on the same graph.



So the thought is that you can expand the sine function around $x=x_0$ to obtain the equations you need. Then, using Laplacian transforms, $x_1 and x_2$ are solvable.










share|cite|improve this question











$endgroup$



closed as off-topic by MisterRiemann, the_candyman, Davide Giraudo, amWhy, KReiser Dec 8 '18 at 0:22


This question appears to be off-topic. The users who voted to close gave this specific reason:


  • "This question is missing context or other details: Please provide additional context, which ideally explains why the question is relevant to you and our community. Some forms of context include: background and motivation, relevant definitions, source, possible strategies, your current progress, why the question is interesting or important, etc." – MisterRiemann, Davide Giraudo, amWhy, KReiser

If this question can be reworded to fit the rules in the help center, please edit the question.













  • $begingroup$
    What is $x_0, x_1$ and $x_2$? Please, provide more details. Most importantly, add also your efforts. Otherwise, I feel that this question will be closed soon and you won't get any answer.
    $endgroup$
    – the_candyman
    Dec 7 '18 at 18:14










  • $begingroup$
    Where did you find this, or what prompted you to conceive it? It it essential that ε be small? And is there some slick answer? I would say it's not massively different from SHM, as when x gets to the domain in which sine levels-off, it will still be follwing a downward-curving parabola.
    $endgroup$
    – AmbretteOrrisey
    Dec 7 '18 at 18:38












  • $begingroup$
    Whoops, did not mean to post. I simply wanted to save for later. Regardless, I updated with more information and direction that I am headed.
    $endgroup$
    – Pascal
    Dec 7 '18 at 20:12






  • 2




    $begingroup$
    @Pascal -- I've done that! It's easy, isn't it, when you're using the fields here as your personal equation-editor ... but who would be so delinquent as to do a thing like that!!? ¶ Whhoops! I've just said ... I've done it!!
    $endgroup$
    – AmbretteOrrisey
    Dec 7 '18 at 20:48
















-1












-1








-1





$begingroup$


Consider the nonlinear equation
$$frac{d^2x}{dt^2}+epsilonsin(x)=0,~~epsilon ll 1\
x(0)=0,~~dot{x}(0)=1$$



and find...

A. The value of $x_0$ as $epsilon$ goes to $0$

B. The first order term $x_1$ and the second order term $x_2$

C. Plot $x(t)$ for $x_0$, $x_1$, and $x_2$

D. Assemble the solution $x=x_0(t)+epsilon x_1(t)+epsilon^2 x_2(t)$. Plot $x(t)=x_0(t)$, $x=x_0(t)+epsilon x_1(t)$ and $x+x_0(t)+epsilon x_1(t)+epsilon^2 x_2(t)$ on the same graph.



So the thought is that you can expand the sine function around $x=x_0$ to obtain the equations you need. Then, using Laplacian transforms, $x_1 and x_2$ are solvable.










share|cite|improve this question











$endgroup$




Consider the nonlinear equation
$$frac{d^2x}{dt^2}+epsilonsin(x)=0,~~epsilon ll 1\
x(0)=0,~~dot{x}(0)=1$$



and find...

A. The value of $x_0$ as $epsilon$ goes to $0$

B. The first order term $x_1$ and the second order term $x_2$

C. Plot $x(t)$ for $x_0$, $x_1$, and $x_2$

D. Assemble the solution $x=x_0(t)+epsilon x_1(t)+epsilon^2 x_2(t)$. Plot $x(t)=x_0(t)$, $x=x_0(t)+epsilon x_1(t)$ and $x+x_0(t)+epsilon x_1(t)+epsilon^2 x_2(t)$ on the same graph.



So the thought is that you can expand the sine function around $x=x_0$ to obtain the equations you need. Then, using Laplacian transforms, $x_1 and x_2$ are solvable.







calculus linear-algebra ordinary-differential-equations nonlinear-system nonlinear-analysis






share|cite|improve this question















share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








edited Dec 7 '18 at 20:11







Pascal

















asked Dec 7 '18 at 18:03









PascalPascal

15810




15810




closed as off-topic by MisterRiemann, the_candyman, Davide Giraudo, amWhy, KReiser Dec 8 '18 at 0:22


This question appears to be off-topic. The users who voted to close gave this specific reason:


  • "This question is missing context or other details: Please provide additional context, which ideally explains why the question is relevant to you and our community. Some forms of context include: background and motivation, relevant definitions, source, possible strategies, your current progress, why the question is interesting or important, etc." – MisterRiemann, Davide Giraudo, amWhy, KReiser

If this question can be reworded to fit the rules in the help center, please edit the question.




closed as off-topic by MisterRiemann, the_candyman, Davide Giraudo, amWhy, KReiser Dec 8 '18 at 0:22


This question appears to be off-topic. The users who voted to close gave this specific reason:


  • "This question is missing context or other details: Please provide additional context, which ideally explains why the question is relevant to you and our community. Some forms of context include: background and motivation, relevant definitions, source, possible strategies, your current progress, why the question is interesting or important, etc." – MisterRiemann, Davide Giraudo, amWhy, KReiser

If this question can be reworded to fit the rules in the help center, please edit the question.












  • $begingroup$
    What is $x_0, x_1$ and $x_2$? Please, provide more details. Most importantly, add also your efforts. Otherwise, I feel that this question will be closed soon and you won't get any answer.
    $endgroup$
    – the_candyman
    Dec 7 '18 at 18:14










  • $begingroup$
    Where did you find this, or what prompted you to conceive it? It it essential that ε be small? And is there some slick answer? I would say it's not massively different from SHM, as when x gets to the domain in which sine levels-off, it will still be follwing a downward-curving parabola.
    $endgroup$
    – AmbretteOrrisey
    Dec 7 '18 at 18:38












  • $begingroup$
    Whoops, did not mean to post. I simply wanted to save for later. Regardless, I updated with more information and direction that I am headed.
    $endgroup$
    – Pascal
    Dec 7 '18 at 20:12






  • 2




    $begingroup$
    @Pascal -- I've done that! It's easy, isn't it, when you're using the fields here as your personal equation-editor ... but who would be so delinquent as to do a thing like that!!? ¶ Whhoops! I've just said ... I've done it!!
    $endgroup$
    – AmbretteOrrisey
    Dec 7 '18 at 20:48




















  • $begingroup$
    What is $x_0, x_1$ and $x_2$? Please, provide more details. Most importantly, add also your efforts. Otherwise, I feel that this question will be closed soon and you won't get any answer.
    $endgroup$
    – the_candyman
    Dec 7 '18 at 18:14










  • $begingroup$
    Where did you find this, or what prompted you to conceive it? It it essential that ε be small? And is there some slick answer? I would say it's not massively different from SHM, as when x gets to the domain in which sine levels-off, it will still be follwing a downward-curving parabola.
    $endgroup$
    – AmbretteOrrisey
    Dec 7 '18 at 18:38












  • $begingroup$
    Whoops, did not mean to post. I simply wanted to save for later. Regardless, I updated with more information and direction that I am headed.
    $endgroup$
    – Pascal
    Dec 7 '18 at 20:12






  • 2




    $begingroup$
    @Pascal -- I've done that! It's easy, isn't it, when you're using the fields here as your personal equation-editor ... but who would be so delinquent as to do a thing like that!!? ¶ Whhoops! I've just said ... I've done it!!
    $endgroup$
    – AmbretteOrrisey
    Dec 7 '18 at 20:48


















$begingroup$
What is $x_0, x_1$ and $x_2$? Please, provide more details. Most importantly, add also your efforts. Otherwise, I feel that this question will be closed soon and you won't get any answer.
$endgroup$
– the_candyman
Dec 7 '18 at 18:14




$begingroup$
What is $x_0, x_1$ and $x_2$? Please, provide more details. Most importantly, add also your efforts. Otherwise, I feel that this question will be closed soon and you won't get any answer.
$endgroup$
– the_candyman
Dec 7 '18 at 18:14












$begingroup$
Where did you find this, or what prompted you to conceive it? It it essential that ε be small? And is there some slick answer? I would say it's not massively different from SHM, as when x gets to the domain in which sine levels-off, it will still be follwing a downward-curving parabola.
$endgroup$
– AmbretteOrrisey
Dec 7 '18 at 18:38






$begingroup$
Where did you find this, or what prompted you to conceive it? It it essential that ε be small? And is there some slick answer? I would say it's not massively different from SHM, as when x gets to the domain in which sine levels-off, it will still be follwing a downward-curving parabola.
$endgroup$
– AmbretteOrrisey
Dec 7 '18 at 18:38














$begingroup$
Whoops, did not mean to post. I simply wanted to save for later. Regardless, I updated with more information and direction that I am headed.
$endgroup$
– Pascal
Dec 7 '18 at 20:12




$begingroup$
Whoops, did not mean to post. I simply wanted to save for later. Regardless, I updated with more information and direction that I am headed.
$endgroup$
– Pascal
Dec 7 '18 at 20:12




2




2




$begingroup$
@Pascal -- I've done that! It's easy, isn't it, when you're using the fields here as your personal equation-editor ... but who would be so delinquent as to do a thing like that!!? ¶ Whhoops! I've just said ... I've done it!!
$endgroup$
– AmbretteOrrisey
Dec 7 '18 at 20:48






$begingroup$
@Pascal -- I've done that! It's easy, isn't it, when you're using the fields here as your personal equation-editor ... but who would be so delinquent as to do a thing like that!!? ¶ Whhoops! I've just said ... I've done it!!
$endgroup$
– AmbretteOrrisey
Dec 7 '18 at 20:48












1 Answer
1






active

oldest

votes


















1












$begingroup$

You have to solve for the terms in $x=x_0+ϵx_1+ϵ^2x_2+...$, so that comparing the powers of $ϵ$ you get
$$
ddot x_0=0,~~x_0(0)=0,~dot x_0(0)=1\
ddot x_1=-sin x_0,~~x_1(0)=0,~dot x_1(0)=0\
ddot x_2=-cos(x_0),x_1,~~x_2(0)=0,~dot x_2(0)=0\
$$





In another approach, multiply with $2dot x$ and integrate to find
$$
1=dot x^2+2ϵ(1-cos x)=dot x^2+4ϵsin^2frac x2
$$

This is a circle equation that can be parametrized via $dot x=cosphi(t)$, $2sqrtϵsinfrac x2=sinphi(t)$ or $x=2arcsinfrac{sinphi(t)}{2sqrtϵ}$. Compare the expressions for the first derivative
$$
cosϕ(t)=dot x=frac{cosϕ(t),dot ϕ(t)}{sqrt{ϵ-frac14sin^2ϕ(t)}}
$$

Now you can expand $1=dot ϕ(t)left(ϵ-frac14sin^2ϕ(t)right)^{-1/2}$ in powers of $ϵ$ and integrate.






share|cite|improve this answer











$endgroup$




















    1 Answer
    1






    active

    oldest

    votes








    1 Answer
    1






    active

    oldest

    votes









    active

    oldest

    votes






    active

    oldest

    votes









    1












    $begingroup$

    You have to solve for the terms in $x=x_0+ϵx_1+ϵ^2x_2+...$, so that comparing the powers of $ϵ$ you get
    $$
    ddot x_0=0,~~x_0(0)=0,~dot x_0(0)=1\
    ddot x_1=-sin x_0,~~x_1(0)=0,~dot x_1(0)=0\
    ddot x_2=-cos(x_0),x_1,~~x_2(0)=0,~dot x_2(0)=0\
    $$





    In another approach, multiply with $2dot x$ and integrate to find
    $$
    1=dot x^2+2ϵ(1-cos x)=dot x^2+4ϵsin^2frac x2
    $$

    This is a circle equation that can be parametrized via $dot x=cosphi(t)$, $2sqrtϵsinfrac x2=sinphi(t)$ or $x=2arcsinfrac{sinphi(t)}{2sqrtϵ}$. Compare the expressions for the first derivative
    $$
    cosϕ(t)=dot x=frac{cosϕ(t),dot ϕ(t)}{sqrt{ϵ-frac14sin^2ϕ(t)}}
    $$

    Now you can expand $1=dot ϕ(t)left(ϵ-frac14sin^2ϕ(t)right)^{-1/2}$ in powers of $ϵ$ and integrate.






    share|cite|improve this answer











    $endgroup$


















      1












      $begingroup$

      You have to solve for the terms in $x=x_0+ϵx_1+ϵ^2x_2+...$, so that comparing the powers of $ϵ$ you get
      $$
      ddot x_0=0,~~x_0(0)=0,~dot x_0(0)=1\
      ddot x_1=-sin x_0,~~x_1(0)=0,~dot x_1(0)=0\
      ddot x_2=-cos(x_0),x_1,~~x_2(0)=0,~dot x_2(0)=0\
      $$





      In another approach, multiply with $2dot x$ and integrate to find
      $$
      1=dot x^2+2ϵ(1-cos x)=dot x^2+4ϵsin^2frac x2
      $$

      This is a circle equation that can be parametrized via $dot x=cosphi(t)$, $2sqrtϵsinfrac x2=sinphi(t)$ or $x=2arcsinfrac{sinphi(t)}{2sqrtϵ}$. Compare the expressions for the first derivative
      $$
      cosϕ(t)=dot x=frac{cosϕ(t),dot ϕ(t)}{sqrt{ϵ-frac14sin^2ϕ(t)}}
      $$

      Now you can expand $1=dot ϕ(t)left(ϵ-frac14sin^2ϕ(t)right)^{-1/2}$ in powers of $ϵ$ and integrate.






      share|cite|improve this answer











      $endgroup$
















        1












        1








        1





        $begingroup$

        You have to solve for the terms in $x=x_0+ϵx_1+ϵ^2x_2+...$, so that comparing the powers of $ϵ$ you get
        $$
        ddot x_0=0,~~x_0(0)=0,~dot x_0(0)=1\
        ddot x_1=-sin x_0,~~x_1(0)=0,~dot x_1(0)=0\
        ddot x_2=-cos(x_0),x_1,~~x_2(0)=0,~dot x_2(0)=0\
        $$





        In another approach, multiply with $2dot x$ and integrate to find
        $$
        1=dot x^2+2ϵ(1-cos x)=dot x^2+4ϵsin^2frac x2
        $$

        This is a circle equation that can be parametrized via $dot x=cosphi(t)$, $2sqrtϵsinfrac x2=sinphi(t)$ or $x=2arcsinfrac{sinphi(t)}{2sqrtϵ}$. Compare the expressions for the first derivative
        $$
        cosϕ(t)=dot x=frac{cosϕ(t),dot ϕ(t)}{sqrt{ϵ-frac14sin^2ϕ(t)}}
        $$

        Now you can expand $1=dot ϕ(t)left(ϵ-frac14sin^2ϕ(t)right)^{-1/2}$ in powers of $ϵ$ and integrate.






        share|cite|improve this answer











        $endgroup$



        You have to solve for the terms in $x=x_0+ϵx_1+ϵ^2x_2+...$, so that comparing the powers of $ϵ$ you get
        $$
        ddot x_0=0,~~x_0(0)=0,~dot x_0(0)=1\
        ddot x_1=-sin x_0,~~x_1(0)=0,~dot x_1(0)=0\
        ddot x_2=-cos(x_0),x_1,~~x_2(0)=0,~dot x_2(0)=0\
        $$





        In another approach, multiply with $2dot x$ and integrate to find
        $$
        1=dot x^2+2ϵ(1-cos x)=dot x^2+4ϵsin^2frac x2
        $$

        This is a circle equation that can be parametrized via $dot x=cosphi(t)$, $2sqrtϵsinfrac x2=sinphi(t)$ or $x=2arcsinfrac{sinphi(t)}{2sqrtϵ}$. Compare the expressions for the first derivative
        $$
        cosϕ(t)=dot x=frac{cosϕ(t),dot ϕ(t)}{sqrt{ϵ-frac14sin^2ϕ(t)}}
        $$

        Now you can expand $1=dot ϕ(t)left(ϵ-frac14sin^2ϕ(t)right)^{-1/2}$ in powers of $ϵ$ and integrate.







        share|cite|improve this answer














        share|cite|improve this answer



        share|cite|improve this answer








        edited Dec 7 '18 at 19:25

























        answered Dec 7 '18 at 19:17









        LutzLLutzL

        57.3k42054




        57.3k42054















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