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Parts V, VI and VII of this study are dedicated to the computation of paraxial rays and dynamic characteristics along the stationary rays obtained numerically in Part III. In this part (Part V), we formulate the linear, second-order, Jacobi dynamic ray tracing equation. In Part VI, we compare the Lagrangian and Hamiltonian approaches to the dynamic ray tracing in heterogeneous isotropic and anisotropic media; we demonstrate that the two approaches are compatible and derive the relationships between the Lagrangian's and Hamiltonian's Hessian matrices. In Part VII, we apply a similar finite-element solver, as used for the kinematic ray tracing, to compute the dynamic characteristics between the source and any point along the ray. The dynamic characteristics in our study include the relative geometric spreading and the phase correction factor due to caustics (i.e., the amplitude and the phase of the Green's function of waves propagating in 3D heterogeneous anisotropic media). The basic solution of the Jacobi equation is a shift vector of a paraxial ray in the plane normal to the ray direction at each point along the central ray. A general paraxial ray is defined by a linear combination of up to four basic vector solutions, each corresponds to specific initial conditions related to the ray coordinates at the source. We define the four basic solutions with two pairs of initial condition sets: point-source and plane-wave. For the proposed point-source ray coordinates and initial conditions, we derive the ray Jacobian and relate it to the relative geometric spreading for general anisotropy. Finally, we introduce a new dynamic parameter, referred as the normalized geometrical spreading, considered a measure of complexity of the propagated wave/ray phenomena, and hence, we propose using a criterion based on this parameter as a qualifying factor associated with the given ray solution.