A free motion equation is a differential equation that describes a mechanical system in the absence of external forces, but in the presence only of an inertial force depending on the choice of a reference frame. In non-autonomous mechanics on a configuration space                     Q        →                  R                        , a free motion equation is defined as a second order non-autonomous dynamic equation on                     Q        →                  R                         which is brought into the form
                                                        q              ¯                                            t            t                                i                          =        0                with respect to some reference frame                     (        t        ,                                            q              ¯                                            i                          )                 on                     Q        →                  R                        . Given an arbitrary reference frame                     (        t        ,                  q                      i                          )                 on                     Q        →                  R                        , a free motion equation reads
                              q                      t            t                                i                          =                  d                      t                                    Γ                      i                          +                  ∂                      j                                    Γ                      i                          (                  q                      t                                j                          −                  Γ                      j                          )        −                                            ∂                              q                                  i                                                                    ∂                                                                    q                    ¯                                                                    m                                                                                                        ∂                                                                    q                    ¯                                                                    m                                                                    ∂                              q                                  j                                            ∂                              q                                  k                                                                    (                  q                      t                                j                          −                  Γ                      j                          )        (                  q                      t                                k                          −                  Γ                      k                          )        ,                where                               Γ                      i                          =                  ∂                      t                                    q                      i                          (        t        ,                                            q              ¯                                            j                          )                 is a connection on                     Q        →                  R                         associates with the initial reference frame                     (        t        ,                                            q              ¯                                            i                          )                . The right-hand side of this equation is treated as an inertial force.
A free motion equation need not exist in general. It can be defined if and only if a configuration bundle                     Q        →                  R                         of a mechanical system is a toroidal cylinder                               T                      m                          ×                              R                                k                                  .