• Source: Non-autonomous system (mathematics)
    • In mathematics, an autonomous system is a dynamic equation on a smooth manifold. A non-autonomous system is a dynamic equation on a smooth fiber bundle



      Q


      R



      {\displaystyle Q\to \mathbb {R} }

      over




      R



      {\displaystyle \mathbb {R} }

      . For instance, this is the case of non-autonomous mechanics.
      An r-order differential equation on a fiber bundle



      Q


      R



      {\displaystyle Q\to \mathbb {R} }

      is represented by a closed subbundle of a jet bundle




      J

      r


      Q


      {\displaystyle J^{r}Q}

      of



      Q


      R



      {\displaystyle Q\to \mathbb {R} }

      . A dynamic equation on



      Q


      R



      {\displaystyle Q\to \mathbb {R} }

      is a differential equation which is algebraically solved for a higher-order derivatives.
      In particular, a first-order dynamic equation on a fiber bundle



      Q


      R



      {\displaystyle Q\to \mathbb {R} }

      is a kernel of the covariant differential of some connection



      Γ


      {\displaystyle \Gamma }

      on



      Q


      R



      {\displaystyle Q\to \mathbb {R} }

      . Given bundle coordinates



      (
      t
      ,

      q

      i


      )


      {\displaystyle (t,q^{i})}

      on



      Q


      {\displaystyle Q}

      and the adapted coordinates



      (
      t
      ,

      q

      i


      ,

      q

      t


      i


      )


      {\displaystyle (t,q^{i},q_{t}^{i})}

      on a first-order jet manifold




      J

      1


      Q


      {\displaystyle J^{1}Q}

      , a first-order dynamic equation reads





      q

      t


      i


      =
      Γ
      (
      t
      ,

      q

      i


      )
      .


      {\displaystyle q_{t}^{i}=\Gamma (t,q^{i}).}


      For instance, this is the case of Hamiltonian non-autonomous mechanics.
      A second-order dynamic equation





      q

      t
      t


      i


      =

      ξ

      i


      (
      t
      ,

      q

      j


      ,

      q

      t


      j


      )


      {\displaystyle q_{tt}^{i}=\xi ^{i}(t,q^{j},q_{t}^{j})}


      on



      Q


      R



      {\displaystyle Q\to \mathbb {R} }

      is defined as a holonomic
      connection



      ξ


      {\displaystyle \xi }

      on a jet bundle




      J

      1


      Q


      R



      {\displaystyle J^{1}Q\to \mathbb {R} }

      . This
      equation also is represented by a connection on an affine jet bundle




      J

      1


      Q

      Q


      {\displaystyle J^{1}Q\to Q}

      . Due to the canonical
      embedding




      J

      1


      Q

      T
      Q


      {\displaystyle J^{1}Q\to TQ}

      , it is equivalent to a geodesic equation
      on the tangent bundle



      T
      Q


      {\displaystyle TQ}

      of



      Q


      {\displaystyle Q}

      . A free motion equation in non-autonomous mechanics exemplifies a second-order non-autonomous dynamic equation.


      See also


      Autonomous system (mathematics)
      Non-autonomous mechanics
      Free motion equation
      Relativistic system (mathematics)


      References


      De Leon, M., Rodrigues, P., Methods of Differential Geometry in Analytical Mechanics (North Holland, 1989).
      Giachetta, G., Mangiarotti, L., Sardanashvily, G., Geometric Formulation of Classical and Quantum Mechanics (World Scientific, 2010) ISBN 981-4313-72-6 (arXiv:0911.0411).

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