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What are differential equations and how do you solve ${dy over dx}=y$ and find $y$ in terms $x$?


How do you solve differential equations in the form of $ay'' + by' +cy = d$?How do you solve second-order linear differential equations without inspection?how to solve second order differential equationFind the maximum area of a right triangle with a constant perimeter P.How do you know when to use the Chain Rule instead of the Power Rule?What method should I apply to solve this differential equation?How to solve differential equations that look like theseSolve System of Differential equations w/o using matrices.How to solve differential equation with one differential termFind the integrating factor and solve













-1












$begingroup$


I had been wondering about how to solve the equation $${dy over dx}=y$$. My progress was to use the chain rule, like setting $$z=2x;{dyover dx}={dyover dz}*{dzover dx}={dyover d(2x)}*2=y.$$ Now I’m officially stuck. What am I supposed to do?
An answer that do work(just for checking): $e^{x+1}$










share|cite|improve this question









$endgroup$








  • 1




    $begingroup$
    e$^x$ also works
    $endgroup$
    – J. W. Tanner
    Mar 10 at 14:20






  • 2




    $begingroup$
    $int {dy over y} = int dx$
    $endgroup$
    – J. W. Tanner
    Mar 10 at 14:21










  • $begingroup$
    it's variable separable ODE also linear .
    $endgroup$
    – Faraday Pathak
    Mar 10 at 14:26












  • $begingroup$
    @J.W.Tanner I know that.
    $endgroup$
    – Math Lover
    Mar 10 at 23:46












  • $begingroup$
    THANKS A LOT FOR YOUR ANSWERS!
    $endgroup$
    – Math Lover
    Mar 10 at 23:50
















-1












$begingroup$


I had been wondering about how to solve the equation $${dy over dx}=y$$. My progress was to use the chain rule, like setting $$z=2x;{dyover dx}={dyover dz}*{dzover dx}={dyover d(2x)}*2=y.$$ Now I’m officially stuck. What am I supposed to do?
An answer that do work(just for checking): $e^{x+1}$










share|cite|improve this question









$endgroup$








  • 1




    $begingroup$
    e$^x$ also works
    $endgroup$
    – J. W. Tanner
    Mar 10 at 14:20






  • 2




    $begingroup$
    $int {dy over y} = int dx$
    $endgroup$
    – J. W. Tanner
    Mar 10 at 14:21










  • $begingroup$
    it's variable separable ODE also linear .
    $endgroup$
    – Faraday Pathak
    Mar 10 at 14:26












  • $begingroup$
    @J.W.Tanner I know that.
    $endgroup$
    – Math Lover
    Mar 10 at 23:46












  • $begingroup$
    THANKS A LOT FOR YOUR ANSWERS!
    $endgroup$
    – Math Lover
    Mar 10 at 23:50














-1












-1








-1


1



$begingroup$


I had been wondering about how to solve the equation $${dy over dx}=y$$. My progress was to use the chain rule, like setting $$z=2x;{dyover dx}={dyover dz}*{dzover dx}={dyover d(2x)}*2=y.$$ Now I’m officially stuck. What am I supposed to do?
An answer that do work(just for checking): $e^{x+1}$










share|cite|improve this question









$endgroup$




I had been wondering about how to solve the equation $${dy over dx}=y$$. My progress was to use the chain rule, like setting $$z=2x;{dyover dx}={dyover dz}*{dzover dx}={dyover d(2x)}*2=y.$$ Now I’m officially stuck. What am I supposed to do?
An answer that do work(just for checking): $e^{x+1}$







ordinary-differential-equations derivatives exponential-function chain-rule






share|cite|improve this question













share|cite|improve this question











share|cite|improve this question




share|cite|improve this question










asked Mar 10 at 14:18









Math LoverMath Lover

16010




16010








  • 1




    $begingroup$
    e$^x$ also works
    $endgroup$
    – J. W. Tanner
    Mar 10 at 14:20






  • 2




    $begingroup$
    $int {dy over y} = int dx$
    $endgroup$
    – J. W. Tanner
    Mar 10 at 14:21










  • $begingroup$
    it's variable separable ODE also linear .
    $endgroup$
    – Faraday Pathak
    Mar 10 at 14:26












  • $begingroup$
    @J.W.Tanner I know that.
    $endgroup$
    – Math Lover
    Mar 10 at 23:46












  • $begingroup$
    THANKS A LOT FOR YOUR ANSWERS!
    $endgroup$
    – Math Lover
    Mar 10 at 23:50














  • 1




    $begingroup$
    e$^x$ also works
    $endgroup$
    – J. W. Tanner
    Mar 10 at 14:20






  • 2




    $begingroup$
    $int {dy over y} = int dx$
    $endgroup$
    – J. W. Tanner
    Mar 10 at 14:21










  • $begingroup$
    it's variable separable ODE also linear .
    $endgroup$
    – Faraday Pathak
    Mar 10 at 14:26












  • $begingroup$
    @J.W.Tanner I know that.
    $endgroup$
    – Math Lover
    Mar 10 at 23:46












  • $begingroup$
    THANKS A LOT FOR YOUR ANSWERS!
    $endgroup$
    – Math Lover
    Mar 10 at 23:50








1




1




$begingroup$
e$^x$ also works
$endgroup$
– J. W. Tanner
Mar 10 at 14:20




$begingroup$
e$^x$ also works
$endgroup$
– J. W. Tanner
Mar 10 at 14:20




2




2




$begingroup$
$int {dy over y} = int dx$
$endgroup$
– J. W. Tanner
Mar 10 at 14:21




$begingroup$
$int {dy over y} = int dx$
$endgroup$
– J. W. Tanner
Mar 10 at 14:21












$begingroup$
it's variable separable ODE also linear .
$endgroup$
– Faraday Pathak
Mar 10 at 14:26






$begingroup$
it's variable separable ODE also linear .
$endgroup$
– Faraday Pathak
Mar 10 at 14:26














$begingroup$
@J.W.Tanner I know that.
$endgroup$
– Math Lover
Mar 10 at 23:46






$begingroup$
@J.W.Tanner I know that.
$endgroup$
– Math Lover
Mar 10 at 23:46














$begingroup$
THANKS A LOT FOR YOUR ANSWERS!
$endgroup$
– Math Lover
Mar 10 at 23:50




$begingroup$
THANKS A LOT FOR YOUR ANSWERS!
$endgroup$
– Math Lover
Mar 10 at 23:50










4 Answers
4






active

oldest

votes


















1












$begingroup$

This is a separable differential equation. Assuming $yne0$ which is a condition we will check separately, divide both sides of the equation by $y$:



$$
frac{dy}{dx}=y\
frac{1}{y}frac{dy}{dx}=1\
intfrac{1}{y}frac{dy}{dx},dx=int,dx\
intfrac{1}{y},dy=x+C_1\
ln{|y|}+C_2=x+C_1\
ln{|y|}=x+C_1-C_2\
ln{|y|}=x+C_3\
|y|=e^{x+C_3}\
y=pm e^{C_3}e^{x}
$$



$pm e^{C_3}$ covers all real numbers except $0$. But $y=0$ is also a solution because $0'=0$. Therefore, we can write the following as the general solution to this equation:



$$y=Ce^x, Cinmathbb{R}.$$






share|cite|improve this answer











$endgroup$





















    4












    $begingroup$

    $frac{dy}{dx}=yRightarrowfrac{dy}{y}=dxRightarrowintfrac{dy}{y}=int dx$



    $Rightarrow lnleft(yright)=x+CRightarrow y=e^{x+C}=C'e^x$



    $C$ and $C'=e^{C}$ are constants; in order to put integrals, you should quote the theorem of separation of variables for differential equations.






    share|cite|improve this answer










    New contributor




    Jack Talion is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
    Check out our Code of Conduct.






    $endgroup$













    • $begingroup$
      I corrected $C’e$ to $C’e^x$
      $endgroup$
      – J. W. Tanner
      Mar 10 at 14:45










    • $begingroup$
      My mistake typing it, thank you!
      $endgroup$
      – Jack Talion
      Mar 10 at 14:46



















    1












    $begingroup$

    Here comes a solution without "magical" manipulation of differentials.



    Assuming that $y neq 0$ on some interval, divide the equation with $y$:
    $$frac{y'(x)}{y(x)} = 1.$$



    Now the left hand side can be written as the derivative of $ln |y(x)|$ and the right hand side as the derivative of $x$:
    $$frac{d}{dx} ln |y(x)| = frac{d}{dx} x.$$



    Therefore, $ln |y(x)| = x + C,$ where $C$ is some constant, and on the interval we thus have
    $$y(x) = pm e^{x+C} = pm e^C e^x = C' e^x,$$
    where $C' = pm e^C$ is a nonzero constant.



    We can see though that also when $C' = 0,$ we get a solution: $y(x) equiv 0.$ We therefore have a general solution $y(x) = C' e^x,$ where $C'$ is a constant.






    share|cite|improve this answer









    $endgroup$





















      1












      $begingroup$

      The first question in your title is




      What are differential equations?




      The informal answer is that often what we know about a quantity we are interested in is its rate of change. For example, if you know the velocity as a function $v(t)$ of time you can find the position $p$ by solving the differential equation
      $$
      p'(t) = v(t) .
      $$

      That's just integration. You use any known position to find the "constant of integration".



      The differential equation you ask about,
      $$
      y' = y,
      $$

      says that the rate of change of $y$ is $y$ itself. In slightly more generality
      $$
      y' = ky
      $$

      says that the rate of change of $y$ is proportional to $y$. That classic equation models population growth over time or compound interest: the more stuff there is the faster it's growing. The solution is exponential growth:
      $$
      y = Ce^{kt}.
      $$



      The second order differential equation
      $$
      y" = -ky
      $$

      models a spring: the second derivative of position is (essentially) a force (that's Newton's law $F=ma$). The equation says that the farther $y$ is from $0$ the greater the force returning it to $0$. The solutions are the oscillating functions $y = sin(t+ phi)$.






      share|cite|improve this answer









      $endgroup$













        Your Answer





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        4 Answers
        4






        active

        oldest

        votes








        4 Answers
        4






        active

        oldest

        votes









        active

        oldest

        votes






        active

        oldest

        votes









        1












        $begingroup$

        This is a separable differential equation. Assuming $yne0$ which is a condition we will check separately, divide both sides of the equation by $y$:



        $$
        frac{dy}{dx}=y\
        frac{1}{y}frac{dy}{dx}=1\
        intfrac{1}{y}frac{dy}{dx},dx=int,dx\
        intfrac{1}{y},dy=x+C_1\
        ln{|y|}+C_2=x+C_1\
        ln{|y|}=x+C_1-C_2\
        ln{|y|}=x+C_3\
        |y|=e^{x+C_3}\
        y=pm e^{C_3}e^{x}
        $$



        $pm e^{C_3}$ covers all real numbers except $0$. But $y=0$ is also a solution because $0'=0$. Therefore, we can write the following as the general solution to this equation:



        $$y=Ce^x, Cinmathbb{R}.$$






        share|cite|improve this answer











        $endgroup$


















          1












          $begingroup$

          This is a separable differential equation. Assuming $yne0$ which is a condition we will check separately, divide both sides of the equation by $y$:



          $$
          frac{dy}{dx}=y\
          frac{1}{y}frac{dy}{dx}=1\
          intfrac{1}{y}frac{dy}{dx},dx=int,dx\
          intfrac{1}{y},dy=x+C_1\
          ln{|y|}+C_2=x+C_1\
          ln{|y|}=x+C_1-C_2\
          ln{|y|}=x+C_3\
          |y|=e^{x+C_3}\
          y=pm e^{C_3}e^{x}
          $$



          $pm e^{C_3}$ covers all real numbers except $0$. But $y=0$ is also a solution because $0'=0$. Therefore, we can write the following as the general solution to this equation:



          $$y=Ce^x, Cinmathbb{R}.$$






          share|cite|improve this answer











          $endgroup$
















            1












            1








            1





            $begingroup$

            This is a separable differential equation. Assuming $yne0$ which is a condition we will check separately, divide both sides of the equation by $y$:



            $$
            frac{dy}{dx}=y\
            frac{1}{y}frac{dy}{dx}=1\
            intfrac{1}{y}frac{dy}{dx},dx=int,dx\
            intfrac{1}{y},dy=x+C_1\
            ln{|y|}+C_2=x+C_1\
            ln{|y|}=x+C_1-C_2\
            ln{|y|}=x+C_3\
            |y|=e^{x+C_3}\
            y=pm e^{C_3}e^{x}
            $$



            $pm e^{C_3}$ covers all real numbers except $0$. But $y=0$ is also a solution because $0'=0$. Therefore, we can write the following as the general solution to this equation:



            $$y=Ce^x, Cinmathbb{R}.$$






            share|cite|improve this answer











            $endgroup$



            This is a separable differential equation. Assuming $yne0$ which is a condition we will check separately, divide both sides of the equation by $y$:



            $$
            frac{dy}{dx}=y\
            frac{1}{y}frac{dy}{dx}=1\
            intfrac{1}{y}frac{dy}{dx},dx=int,dx\
            intfrac{1}{y},dy=x+C_1\
            ln{|y|}+C_2=x+C_1\
            ln{|y|}=x+C_1-C_2\
            ln{|y|}=x+C_3\
            |y|=e^{x+C_3}\
            y=pm e^{C_3}e^{x}
            $$



            $pm e^{C_3}$ covers all real numbers except $0$. But $y=0$ is also a solution because $0'=0$. Therefore, we can write the following as the general solution to this equation:



            $$y=Ce^x, Cinmathbb{R}.$$







            share|cite|improve this answer














            share|cite|improve this answer



            share|cite|improve this answer








            edited Mar 11 at 1:08









            J. W. Tanner

            3,2401320




            3,2401320










            answered Mar 10 at 16:40









            Michael RybkinMichael Rybkin

            3,884420




            3,884420























                4












                $begingroup$

                $frac{dy}{dx}=yRightarrowfrac{dy}{y}=dxRightarrowintfrac{dy}{y}=int dx$



                $Rightarrow lnleft(yright)=x+CRightarrow y=e^{x+C}=C'e^x$



                $C$ and $C'=e^{C}$ are constants; in order to put integrals, you should quote the theorem of separation of variables for differential equations.






                share|cite|improve this answer










                New contributor




                Jack Talion is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
                Check out our Code of Conduct.






                $endgroup$













                • $begingroup$
                  I corrected $C’e$ to $C’e^x$
                  $endgroup$
                  – J. W. Tanner
                  Mar 10 at 14:45










                • $begingroup$
                  My mistake typing it, thank you!
                  $endgroup$
                  – Jack Talion
                  Mar 10 at 14:46
















                4












                $begingroup$

                $frac{dy}{dx}=yRightarrowfrac{dy}{y}=dxRightarrowintfrac{dy}{y}=int dx$



                $Rightarrow lnleft(yright)=x+CRightarrow y=e^{x+C}=C'e^x$



                $C$ and $C'=e^{C}$ are constants; in order to put integrals, you should quote the theorem of separation of variables for differential equations.






                share|cite|improve this answer










                New contributor




                Jack Talion is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
                Check out our Code of Conduct.






                $endgroup$













                • $begingroup$
                  I corrected $C’e$ to $C’e^x$
                  $endgroup$
                  – J. W. Tanner
                  Mar 10 at 14:45










                • $begingroup$
                  My mistake typing it, thank you!
                  $endgroup$
                  – Jack Talion
                  Mar 10 at 14:46














                4












                4








                4





                $begingroup$

                $frac{dy}{dx}=yRightarrowfrac{dy}{y}=dxRightarrowintfrac{dy}{y}=int dx$



                $Rightarrow lnleft(yright)=x+CRightarrow y=e^{x+C}=C'e^x$



                $C$ and $C'=e^{C}$ are constants; in order to put integrals, you should quote the theorem of separation of variables for differential equations.






                share|cite|improve this answer










                New contributor




                Jack Talion is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
                Check out our Code of Conduct.






                $endgroup$



                $frac{dy}{dx}=yRightarrowfrac{dy}{y}=dxRightarrowintfrac{dy}{y}=int dx$



                $Rightarrow lnleft(yright)=x+CRightarrow y=e^{x+C}=C'e^x$



                $C$ and $C'=e^{C}$ are constants; in order to put integrals, you should quote the theorem of separation of variables for differential equations.







                share|cite|improve this answer










                New contributor




                Jack Talion is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
                Check out our Code of Conduct.









                share|cite|improve this answer



                share|cite|improve this answer








                edited Mar 10 at 16:24









                J. W. Tanner

                3,2401320




                3,2401320






                New contributor




                Jack Talion is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
                Check out our Code of Conduct.









                answered Mar 10 at 14:26









                Jack TalionJack Talion

                886




                886




                New contributor




                Jack Talion is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
                Check out our Code of Conduct.





                New contributor





                Jack Talion is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
                Check out our Code of Conduct.






                Jack Talion is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
                Check out our Code of Conduct.












                • $begingroup$
                  I corrected $C’e$ to $C’e^x$
                  $endgroup$
                  – J. W. Tanner
                  Mar 10 at 14:45










                • $begingroup$
                  My mistake typing it, thank you!
                  $endgroup$
                  – Jack Talion
                  Mar 10 at 14:46


















                • $begingroup$
                  I corrected $C’e$ to $C’e^x$
                  $endgroup$
                  – J. W. Tanner
                  Mar 10 at 14:45










                • $begingroup$
                  My mistake typing it, thank you!
                  $endgroup$
                  – Jack Talion
                  Mar 10 at 14:46
















                $begingroup$
                I corrected $C’e$ to $C’e^x$
                $endgroup$
                – J. W. Tanner
                Mar 10 at 14:45




                $begingroup$
                I corrected $C’e$ to $C’e^x$
                $endgroup$
                – J. W. Tanner
                Mar 10 at 14:45












                $begingroup$
                My mistake typing it, thank you!
                $endgroup$
                – Jack Talion
                Mar 10 at 14:46




                $begingroup$
                My mistake typing it, thank you!
                $endgroup$
                – Jack Talion
                Mar 10 at 14:46











                1












                $begingroup$

                Here comes a solution without "magical" manipulation of differentials.



                Assuming that $y neq 0$ on some interval, divide the equation with $y$:
                $$frac{y'(x)}{y(x)} = 1.$$



                Now the left hand side can be written as the derivative of $ln |y(x)|$ and the right hand side as the derivative of $x$:
                $$frac{d}{dx} ln |y(x)| = frac{d}{dx} x.$$



                Therefore, $ln |y(x)| = x + C,$ where $C$ is some constant, and on the interval we thus have
                $$y(x) = pm e^{x+C} = pm e^C e^x = C' e^x,$$
                where $C' = pm e^C$ is a nonzero constant.



                We can see though that also when $C' = 0,$ we get a solution: $y(x) equiv 0.$ We therefore have a general solution $y(x) = C' e^x,$ where $C'$ is a constant.






                share|cite|improve this answer









                $endgroup$


















                  1












                  $begingroup$

                  Here comes a solution without "magical" manipulation of differentials.



                  Assuming that $y neq 0$ on some interval, divide the equation with $y$:
                  $$frac{y'(x)}{y(x)} = 1.$$



                  Now the left hand side can be written as the derivative of $ln |y(x)|$ and the right hand side as the derivative of $x$:
                  $$frac{d}{dx} ln |y(x)| = frac{d}{dx} x.$$



                  Therefore, $ln |y(x)| = x + C,$ where $C$ is some constant, and on the interval we thus have
                  $$y(x) = pm e^{x+C} = pm e^C e^x = C' e^x,$$
                  where $C' = pm e^C$ is a nonzero constant.



                  We can see though that also when $C' = 0,$ we get a solution: $y(x) equiv 0.$ We therefore have a general solution $y(x) = C' e^x,$ where $C'$ is a constant.






                  share|cite|improve this answer









                  $endgroup$
















                    1












                    1








                    1





                    $begingroup$

                    Here comes a solution without "magical" manipulation of differentials.



                    Assuming that $y neq 0$ on some interval, divide the equation with $y$:
                    $$frac{y'(x)}{y(x)} = 1.$$



                    Now the left hand side can be written as the derivative of $ln |y(x)|$ and the right hand side as the derivative of $x$:
                    $$frac{d}{dx} ln |y(x)| = frac{d}{dx} x.$$



                    Therefore, $ln |y(x)| = x + C,$ where $C$ is some constant, and on the interval we thus have
                    $$y(x) = pm e^{x+C} = pm e^C e^x = C' e^x,$$
                    where $C' = pm e^C$ is a nonzero constant.



                    We can see though that also when $C' = 0,$ we get a solution: $y(x) equiv 0.$ We therefore have a general solution $y(x) = C' e^x,$ where $C'$ is a constant.






                    share|cite|improve this answer









                    $endgroup$



                    Here comes a solution without "magical" manipulation of differentials.



                    Assuming that $y neq 0$ on some interval, divide the equation with $y$:
                    $$frac{y'(x)}{y(x)} = 1.$$



                    Now the left hand side can be written as the derivative of $ln |y(x)|$ and the right hand side as the derivative of $x$:
                    $$frac{d}{dx} ln |y(x)| = frac{d}{dx} x.$$



                    Therefore, $ln |y(x)| = x + C,$ where $C$ is some constant, and on the interval we thus have
                    $$y(x) = pm e^{x+C} = pm e^C e^x = C' e^x,$$
                    where $C' = pm e^C$ is a nonzero constant.



                    We can see though that also when $C' = 0,$ we get a solution: $y(x) equiv 0.$ We therefore have a general solution $y(x) = C' e^x,$ where $C'$ is a constant.







                    share|cite|improve this answer












                    share|cite|improve this answer



                    share|cite|improve this answer










                    answered Mar 10 at 16:50









                    md2perpemd2perpe

                    8,19611028




                    8,19611028























                        1












                        $begingroup$

                        The first question in your title is




                        What are differential equations?




                        The informal answer is that often what we know about a quantity we are interested in is its rate of change. For example, if you know the velocity as a function $v(t)$ of time you can find the position $p$ by solving the differential equation
                        $$
                        p'(t) = v(t) .
                        $$

                        That's just integration. You use any known position to find the "constant of integration".



                        The differential equation you ask about,
                        $$
                        y' = y,
                        $$

                        says that the rate of change of $y$ is $y$ itself. In slightly more generality
                        $$
                        y' = ky
                        $$

                        says that the rate of change of $y$ is proportional to $y$. That classic equation models population growth over time or compound interest: the more stuff there is the faster it's growing. The solution is exponential growth:
                        $$
                        y = Ce^{kt}.
                        $$



                        The second order differential equation
                        $$
                        y" = -ky
                        $$

                        models a spring: the second derivative of position is (essentially) a force (that's Newton's law $F=ma$). The equation says that the farther $y$ is from $0$ the greater the force returning it to $0$. The solutions are the oscillating functions $y = sin(t+ phi)$.






                        share|cite|improve this answer









                        $endgroup$


















                          1












                          $begingroup$

                          The first question in your title is




                          What are differential equations?




                          The informal answer is that often what we know about a quantity we are interested in is its rate of change. For example, if you know the velocity as a function $v(t)$ of time you can find the position $p$ by solving the differential equation
                          $$
                          p'(t) = v(t) .
                          $$

                          That's just integration. You use any known position to find the "constant of integration".



                          The differential equation you ask about,
                          $$
                          y' = y,
                          $$

                          says that the rate of change of $y$ is $y$ itself. In slightly more generality
                          $$
                          y' = ky
                          $$

                          says that the rate of change of $y$ is proportional to $y$. That classic equation models population growth over time or compound interest: the more stuff there is the faster it's growing. The solution is exponential growth:
                          $$
                          y = Ce^{kt}.
                          $$



                          The second order differential equation
                          $$
                          y" = -ky
                          $$

                          models a spring: the second derivative of position is (essentially) a force (that's Newton's law $F=ma$). The equation says that the farther $y$ is from $0$ the greater the force returning it to $0$. The solutions are the oscillating functions $y = sin(t+ phi)$.






                          share|cite|improve this answer









                          $endgroup$
















                            1












                            1








                            1





                            $begingroup$

                            The first question in your title is




                            What are differential equations?




                            The informal answer is that often what we know about a quantity we are interested in is its rate of change. For example, if you know the velocity as a function $v(t)$ of time you can find the position $p$ by solving the differential equation
                            $$
                            p'(t) = v(t) .
                            $$

                            That's just integration. You use any known position to find the "constant of integration".



                            The differential equation you ask about,
                            $$
                            y' = y,
                            $$

                            says that the rate of change of $y$ is $y$ itself. In slightly more generality
                            $$
                            y' = ky
                            $$

                            says that the rate of change of $y$ is proportional to $y$. That classic equation models population growth over time or compound interest: the more stuff there is the faster it's growing. The solution is exponential growth:
                            $$
                            y = Ce^{kt}.
                            $$



                            The second order differential equation
                            $$
                            y" = -ky
                            $$

                            models a spring: the second derivative of position is (essentially) a force (that's Newton's law $F=ma$). The equation says that the farther $y$ is from $0$ the greater the force returning it to $0$. The solutions are the oscillating functions $y = sin(t+ phi)$.






                            share|cite|improve this answer









                            $endgroup$



                            The first question in your title is




                            What are differential equations?




                            The informal answer is that often what we know about a quantity we are interested in is its rate of change. For example, if you know the velocity as a function $v(t)$ of time you can find the position $p$ by solving the differential equation
                            $$
                            p'(t) = v(t) .
                            $$

                            That's just integration. You use any known position to find the "constant of integration".



                            The differential equation you ask about,
                            $$
                            y' = y,
                            $$

                            says that the rate of change of $y$ is $y$ itself. In slightly more generality
                            $$
                            y' = ky
                            $$

                            says that the rate of change of $y$ is proportional to $y$. That classic equation models population growth over time or compound interest: the more stuff there is the faster it's growing. The solution is exponential growth:
                            $$
                            y = Ce^{kt}.
                            $$



                            The second order differential equation
                            $$
                            y" = -ky
                            $$

                            models a spring: the second derivative of position is (essentially) a force (that's Newton's law $F=ma$). The equation says that the farther $y$ is from $0$ the greater the force returning it to $0$. The solutions are the oscillating functions $y = sin(t+ phi)$.







                            share|cite|improve this answer












                            share|cite|improve this answer



                            share|cite|improve this answer










                            answered Mar 11 at 1:28









                            Ethan BolkerEthan Bolker

                            45k553120




                            45k553120






























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