find the solution of a differential equation












0












$begingroup$


we have a particle in laboratory whose equation of motion is a differential equation as




$ddot{x}(s)+2G(x(s),dot{x}(s))=0$




where




$G=frac{-akcos (kx)}{2}(W+(dot{x}-W)^3)$




with $W=(b+asin kx,0,0)$ in which $a$, $b$, and $k$ are real constant values s.t. $0<a<b$ and $a+b<1$.



I also know that




$1=frac{dot{x}(s)}{1+b+asin kx(s)}$.




Trying to find the solution I found




$x(s)=frac{2}{k}arctan(sqrt{1-(frac{a}{1+b})^2}tan ((s+A)frac{k}{2}(1+b)sqrt{1-(frac{a}{1+b})^2})-frac{a}{1+b})$,




where




$A=frac{2}{k(1+b)}frac{1}{sqrt{1-(frac{a}{1+b})^2}}arctanfrac{frac{a}{1+b}}{sqrt{1-(frac{a}{1+b})^2}}$.




Observe that according to the solution, $x(s)$ is periodic with a period of $frac{2pi}{k}$. Moreover, if I am not wrong, its range is $[-frac{pi}{k},frac{pi}{k}]$



Now the problem is that according to the motion of the particle in the laboratory, the range of the is the interval of $[0,infty)$!



So anyone may have any suggestion how to interpret this solution. If there is any other way to rewrite this solution s.t. it is reasonable with the experience. Any suggestion how to deal with this problem?



Thanks a lot!










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$endgroup$

















    0












    $begingroup$


    we have a particle in laboratory whose equation of motion is a differential equation as




    $ddot{x}(s)+2G(x(s),dot{x}(s))=0$




    where




    $G=frac{-akcos (kx)}{2}(W+(dot{x}-W)^3)$




    with $W=(b+asin kx,0,0)$ in which $a$, $b$, and $k$ are real constant values s.t. $0<a<b$ and $a+b<1$.



    I also know that




    $1=frac{dot{x}(s)}{1+b+asin kx(s)}$.




    Trying to find the solution I found




    $x(s)=frac{2}{k}arctan(sqrt{1-(frac{a}{1+b})^2}tan ((s+A)frac{k}{2}(1+b)sqrt{1-(frac{a}{1+b})^2})-frac{a}{1+b})$,




    where




    $A=frac{2}{k(1+b)}frac{1}{sqrt{1-(frac{a}{1+b})^2}}arctanfrac{frac{a}{1+b}}{sqrt{1-(frac{a}{1+b})^2}}$.




    Observe that according to the solution, $x(s)$ is periodic with a period of $frac{2pi}{k}$. Moreover, if I am not wrong, its range is $[-frac{pi}{k},frac{pi}{k}]$



    Now the problem is that according to the motion of the particle in the laboratory, the range of the is the interval of $[0,infty)$!



    So anyone may have any suggestion how to interpret this solution. If there is any other way to rewrite this solution s.t. it is reasonable with the experience. Any suggestion how to deal with this problem?



    Thanks a lot!










    share|cite|improve this question











    $endgroup$















      0












      0








      0





      $begingroup$


      we have a particle in laboratory whose equation of motion is a differential equation as




      $ddot{x}(s)+2G(x(s),dot{x}(s))=0$




      where




      $G=frac{-akcos (kx)}{2}(W+(dot{x}-W)^3)$




      with $W=(b+asin kx,0,0)$ in which $a$, $b$, and $k$ are real constant values s.t. $0<a<b$ and $a+b<1$.



      I also know that




      $1=frac{dot{x}(s)}{1+b+asin kx(s)}$.




      Trying to find the solution I found




      $x(s)=frac{2}{k}arctan(sqrt{1-(frac{a}{1+b})^2}tan ((s+A)frac{k}{2}(1+b)sqrt{1-(frac{a}{1+b})^2})-frac{a}{1+b})$,




      where




      $A=frac{2}{k(1+b)}frac{1}{sqrt{1-(frac{a}{1+b})^2}}arctanfrac{frac{a}{1+b}}{sqrt{1-(frac{a}{1+b})^2}}$.




      Observe that according to the solution, $x(s)$ is periodic with a period of $frac{2pi}{k}$. Moreover, if I am not wrong, its range is $[-frac{pi}{k},frac{pi}{k}]$



      Now the problem is that according to the motion of the particle in the laboratory, the range of the is the interval of $[0,infty)$!



      So anyone may have any suggestion how to interpret this solution. If there is any other way to rewrite this solution s.t. it is reasonable with the experience. Any suggestion how to deal with this problem?



      Thanks a lot!










      share|cite|improve this question











      $endgroup$




      we have a particle in laboratory whose equation of motion is a differential equation as




      $ddot{x}(s)+2G(x(s),dot{x}(s))=0$




      where




      $G=frac{-akcos (kx)}{2}(W+(dot{x}-W)^3)$




      with $W=(b+asin kx,0,0)$ in which $a$, $b$, and $k$ are real constant values s.t. $0<a<b$ and $a+b<1$.



      I also know that




      $1=frac{dot{x}(s)}{1+b+asin kx(s)}$.




      Trying to find the solution I found




      $x(s)=frac{2}{k}arctan(sqrt{1-(frac{a}{1+b})^2}tan ((s+A)frac{k}{2}(1+b)sqrt{1-(frac{a}{1+b})^2})-frac{a}{1+b})$,




      where




      $A=frac{2}{k(1+b)}frac{1}{sqrt{1-(frac{a}{1+b})^2}}arctanfrac{frac{a}{1+b}}{sqrt{1-(frac{a}{1+b})^2}}$.




      Observe that according to the solution, $x(s)$ is periodic with a period of $frac{2pi}{k}$. Moreover, if I am not wrong, its range is $[-frac{pi}{k},frac{pi}{k}]$



      Now the problem is that according to the motion of the particle in the laboratory, the range of the is the interval of $[0,infty)$!



      So anyone may have any suggestion how to interpret this solution. If there is any other way to rewrite this solution s.t. it is reasonable with the experience. Any suggestion how to deal with this problem?



      Thanks a lot!







      calculus geometry ordinary-differential-equations






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      edited Dec 18 '18 at 16:41









      Travis

      63.8k769151




      63.8k769151










      asked Dec 18 '18 at 14:44









      MajidMajid

      1,8731926




      1,8731926






















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