Using solve_ivp instead of odeint to solve initial problem value












0















Currently, I solve the following ODE system of equations using odeint



dx/dt = (-x + u)/2.0



dy/dt = (-y + x)/5.0



initial conditions: x = 0, y = 0



However, I would like to use solve_ivp which seems to be the recommended option for this type of problems, but honestly I don't know how to adapt the code...



Here is the code I'm using with odeint:



import numpy as np
from scipy.integrate import odeint, solve_ivp
import matplotlib.pyplot as plt

def model(z, t, u):
x = z[0]
y = z[1]
dxdt = (-x + u)/2.0
dydt = (-y + x)/5.0
dzdt = [dxdt, dydt]
return dzdt

def main():
# initial condition
z0 = [0, 0]

# number of time points
n = 401

# time points
t = np.linspace(0, 40, n)

# step input
u = np.zeros(n)
# change to 2.0 at time = 5.0
u[51:] = 2.0

# store solution
x = np.empty_like(t)
y = np.empty_like(t)
# record initial conditions
x[0] = z0[0]
y[0] = z0[1]

# solve ODE
for i in range(1, n):
# span for next time step
tspan = [t[i-1], t[i]]
# solve for next step
z = odeint(model, z0, tspan, args=(u[i],))
# store solution for plotting
x[i] = z[1][0]
y[i] = z[1][1]
# next initial condition
z0 = z[1]

# plot results
plt.plot(t,u,'g:',label='u(t)')
plt.plot(t,x,'b-',label='x(t)')
plt.plot(t,y,'r--',label='y(t)')
plt.ylabel('values')
plt.xlabel('time')
plt.legend(loc='best')
plt.show()

main()









share|improve this question



























    0















    Currently, I solve the following ODE system of equations using odeint



    dx/dt = (-x + u)/2.0



    dy/dt = (-y + x)/5.0



    initial conditions: x = 0, y = 0



    However, I would like to use solve_ivp which seems to be the recommended option for this type of problems, but honestly I don't know how to adapt the code...



    Here is the code I'm using with odeint:



    import numpy as np
    from scipy.integrate import odeint, solve_ivp
    import matplotlib.pyplot as plt

    def model(z, t, u):
    x = z[0]
    y = z[1]
    dxdt = (-x + u)/2.0
    dydt = (-y + x)/5.0
    dzdt = [dxdt, dydt]
    return dzdt

    def main():
    # initial condition
    z0 = [0, 0]

    # number of time points
    n = 401

    # time points
    t = np.linspace(0, 40, n)

    # step input
    u = np.zeros(n)
    # change to 2.0 at time = 5.0
    u[51:] = 2.0

    # store solution
    x = np.empty_like(t)
    y = np.empty_like(t)
    # record initial conditions
    x[0] = z0[0]
    y[0] = z0[1]

    # solve ODE
    for i in range(1, n):
    # span for next time step
    tspan = [t[i-1], t[i]]
    # solve for next step
    z = odeint(model, z0, tspan, args=(u[i],))
    # store solution for plotting
    x[i] = z[1][0]
    y[i] = z[1][1]
    # next initial condition
    z0 = z[1]

    # plot results
    plt.plot(t,u,'g:',label='u(t)')
    plt.plot(t,x,'b-',label='x(t)')
    plt.plot(t,y,'r--',label='y(t)')
    plt.ylabel('values')
    plt.xlabel('time')
    plt.legend(loc='best')
    plt.show()

    main()









    share|improve this question

























      0












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      0








      Currently, I solve the following ODE system of equations using odeint



      dx/dt = (-x + u)/2.0



      dy/dt = (-y + x)/5.0



      initial conditions: x = 0, y = 0



      However, I would like to use solve_ivp which seems to be the recommended option for this type of problems, but honestly I don't know how to adapt the code...



      Here is the code I'm using with odeint:



      import numpy as np
      from scipy.integrate import odeint, solve_ivp
      import matplotlib.pyplot as plt

      def model(z, t, u):
      x = z[0]
      y = z[1]
      dxdt = (-x + u)/2.0
      dydt = (-y + x)/5.0
      dzdt = [dxdt, dydt]
      return dzdt

      def main():
      # initial condition
      z0 = [0, 0]

      # number of time points
      n = 401

      # time points
      t = np.linspace(0, 40, n)

      # step input
      u = np.zeros(n)
      # change to 2.0 at time = 5.0
      u[51:] = 2.0

      # store solution
      x = np.empty_like(t)
      y = np.empty_like(t)
      # record initial conditions
      x[0] = z0[0]
      y[0] = z0[1]

      # solve ODE
      for i in range(1, n):
      # span for next time step
      tspan = [t[i-1], t[i]]
      # solve for next step
      z = odeint(model, z0, tspan, args=(u[i],))
      # store solution for plotting
      x[i] = z[1][0]
      y[i] = z[1][1]
      # next initial condition
      z0 = z[1]

      # plot results
      plt.plot(t,u,'g:',label='u(t)')
      plt.plot(t,x,'b-',label='x(t)')
      plt.plot(t,y,'r--',label='y(t)')
      plt.ylabel('values')
      plt.xlabel('time')
      plt.legend(loc='best')
      plt.show()

      main()









      share|improve this question














      Currently, I solve the following ODE system of equations using odeint



      dx/dt = (-x + u)/2.0



      dy/dt = (-y + x)/5.0



      initial conditions: x = 0, y = 0



      However, I would like to use solve_ivp which seems to be the recommended option for this type of problems, but honestly I don't know how to adapt the code...



      Here is the code I'm using with odeint:



      import numpy as np
      from scipy.integrate import odeint, solve_ivp
      import matplotlib.pyplot as plt

      def model(z, t, u):
      x = z[0]
      y = z[1]
      dxdt = (-x + u)/2.0
      dydt = (-y + x)/5.0
      dzdt = [dxdt, dydt]
      return dzdt

      def main():
      # initial condition
      z0 = [0, 0]

      # number of time points
      n = 401

      # time points
      t = np.linspace(0, 40, n)

      # step input
      u = np.zeros(n)
      # change to 2.0 at time = 5.0
      u[51:] = 2.0

      # store solution
      x = np.empty_like(t)
      y = np.empty_like(t)
      # record initial conditions
      x[0] = z0[0]
      y[0] = z0[1]

      # solve ODE
      for i in range(1, n):
      # span for next time step
      tspan = [t[i-1], t[i]]
      # solve for next step
      z = odeint(model, z0, tspan, args=(u[i],))
      # store solution for plotting
      x[i] = z[1][0]
      y[i] = z[1][1]
      # next initial condition
      z0 = z[1]

      # plot results
      plt.plot(t,u,'g:',label='u(t)')
      plt.plot(t,x,'b-',label='x(t)')
      plt.plot(t,y,'r--',label='y(t)')
      plt.ylabel('values')
      plt.xlabel('time')
      plt.legend(loc='best')
      plt.show()

      main()






      python scipy ode differential-equations






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      asked Nov 21 '18 at 15:26









      Sergio ManchadoSergio Manchado

      484




      484
























          1 Answer
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          0














          It's important that solve_ivp expects f(t, z) as right-hand side of the ODE. If you don't want to change your ode function and also want to pass your parameter u, I recommend to define a wrapper function:



          def model(z, t, u):
          x = z[0]
          y = z[1]
          dxdt = (-x + u)/2.0
          dydt = (-y + x)/5.0
          dzdt = [dxdt, dydt]
          return dzdt

          def odefun(t, z):
          if t < 5:
          return model(z, t, 0)
          else:
          return model(z, t, 2)


          Now it's easy to call solve_ivp:



          def main():
          # initial condition
          z0 = [0, 0]

          # number of time points
          n = 401

          # time points
          t = np.linspace(0, 40, n)

          # step input
          u = np.zeros(n)
          # change to 2.0 at time = 5.0
          u[51:] = 2.0

          res = solve_ivp(fun=odefun, t_span=[0, 40], y0=z0, t_eval=t)
          x = res.y[0, :]
          y = res.y[1, :]

          # plot results
          plt.plot(t,u,'g:',label='u(t)')
          plt.plot(t,x,'b-',label='x(t)')
          plt.plot(t,y,'r--',label='y(t)')
          plt.ylabel('values')
          plt.xlabel('time')
          plt.legend(loc='best')
          plt.show()

          main()


          Note that without passing t_eval=t, the solver will automatically choose the time points inside tspan at which the solution will be stored.






          share|improve this answer























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            1 Answer
            1






            active

            oldest

            votes








            1 Answer
            1






            active

            oldest

            votes









            active

            oldest

            votes






            active

            oldest

            votes









            0














            It's important that solve_ivp expects f(t, z) as right-hand side of the ODE. If you don't want to change your ode function and also want to pass your parameter u, I recommend to define a wrapper function:



            def model(z, t, u):
            x = z[0]
            y = z[1]
            dxdt = (-x + u)/2.0
            dydt = (-y + x)/5.0
            dzdt = [dxdt, dydt]
            return dzdt

            def odefun(t, z):
            if t < 5:
            return model(z, t, 0)
            else:
            return model(z, t, 2)


            Now it's easy to call solve_ivp:



            def main():
            # initial condition
            z0 = [0, 0]

            # number of time points
            n = 401

            # time points
            t = np.linspace(0, 40, n)

            # step input
            u = np.zeros(n)
            # change to 2.0 at time = 5.0
            u[51:] = 2.0

            res = solve_ivp(fun=odefun, t_span=[0, 40], y0=z0, t_eval=t)
            x = res.y[0, :]
            y = res.y[1, :]

            # plot results
            plt.plot(t,u,'g:',label='u(t)')
            plt.plot(t,x,'b-',label='x(t)')
            plt.plot(t,y,'r--',label='y(t)')
            plt.ylabel('values')
            plt.xlabel('time')
            plt.legend(loc='best')
            plt.show()

            main()


            Note that without passing t_eval=t, the solver will automatically choose the time points inside tspan at which the solution will be stored.






            share|improve this answer




























              0














              It's important that solve_ivp expects f(t, z) as right-hand side of the ODE. If you don't want to change your ode function and also want to pass your parameter u, I recommend to define a wrapper function:



              def model(z, t, u):
              x = z[0]
              y = z[1]
              dxdt = (-x + u)/2.0
              dydt = (-y + x)/5.0
              dzdt = [dxdt, dydt]
              return dzdt

              def odefun(t, z):
              if t < 5:
              return model(z, t, 0)
              else:
              return model(z, t, 2)


              Now it's easy to call solve_ivp:



              def main():
              # initial condition
              z0 = [0, 0]

              # number of time points
              n = 401

              # time points
              t = np.linspace(0, 40, n)

              # step input
              u = np.zeros(n)
              # change to 2.0 at time = 5.0
              u[51:] = 2.0

              res = solve_ivp(fun=odefun, t_span=[0, 40], y0=z0, t_eval=t)
              x = res.y[0, :]
              y = res.y[1, :]

              # plot results
              plt.plot(t,u,'g:',label='u(t)')
              plt.plot(t,x,'b-',label='x(t)')
              plt.plot(t,y,'r--',label='y(t)')
              plt.ylabel('values')
              plt.xlabel('time')
              plt.legend(loc='best')
              plt.show()

              main()


              Note that without passing t_eval=t, the solver will automatically choose the time points inside tspan at which the solution will be stored.






              share|improve this answer


























                0












                0








                0







                It's important that solve_ivp expects f(t, z) as right-hand side of the ODE. If you don't want to change your ode function and also want to pass your parameter u, I recommend to define a wrapper function:



                def model(z, t, u):
                x = z[0]
                y = z[1]
                dxdt = (-x + u)/2.0
                dydt = (-y + x)/5.0
                dzdt = [dxdt, dydt]
                return dzdt

                def odefun(t, z):
                if t < 5:
                return model(z, t, 0)
                else:
                return model(z, t, 2)


                Now it's easy to call solve_ivp:



                def main():
                # initial condition
                z0 = [0, 0]

                # number of time points
                n = 401

                # time points
                t = np.linspace(0, 40, n)

                # step input
                u = np.zeros(n)
                # change to 2.0 at time = 5.0
                u[51:] = 2.0

                res = solve_ivp(fun=odefun, t_span=[0, 40], y0=z0, t_eval=t)
                x = res.y[0, :]
                y = res.y[1, :]

                # plot results
                plt.plot(t,u,'g:',label='u(t)')
                plt.plot(t,x,'b-',label='x(t)')
                plt.plot(t,y,'r--',label='y(t)')
                plt.ylabel('values')
                plt.xlabel('time')
                plt.legend(loc='best')
                plt.show()

                main()


                Note that without passing t_eval=t, the solver will automatically choose the time points inside tspan at which the solution will be stored.






                share|improve this answer













                It's important that solve_ivp expects f(t, z) as right-hand side of the ODE. If you don't want to change your ode function and also want to pass your parameter u, I recommend to define a wrapper function:



                def model(z, t, u):
                x = z[0]
                y = z[1]
                dxdt = (-x + u)/2.0
                dydt = (-y + x)/5.0
                dzdt = [dxdt, dydt]
                return dzdt

                def odefun(t, z):
                if t < 5:
                return model(z, t, 0)
                else:
                return model(z, t, 2)


                Now it's easy to call solve_ivp:



                def main():
                # initial condition
                z0 = [0, 0]

                # number of time points
                n = 401

                # time points
                t = np.linspace(0, 40, n)

                # step input
                u = np.zeros(n)
                # change to 2.0 at time = 5.0
                u[51:] = 2.0

                res = solve_ivp(fun=odefun, t_span=[0, 40], y0=z0, t_eval=t)
                x = res.y[0, :]
                y = res.y[1, :]

                # plot results
                plt.plot(t,u,'g:',label='u(t)')
                plt.plot(t,x,'b-',label='x(t)')
                plt.plot(t,y,'r--',label='y(t)')
                plt.ylabel('values')
                plt.xlabel('time')
                plt.legend(loc='best')
                plt.show()

                main()


                Note that without passing t_eval=t, the solver will automatically choose the time points inside tspan at which the solution will be stored.







                share|improve this answer












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                answered Nov 21 '18 at 18:53









                jonijoni

                758157




                758157
































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