Use to label the initial point in phase space. The characteristic equations for a transport equation are and , with and . Since the velocity remains fixed, the ordinary differential equations integrate directly:
This characteristic flow map exists for all real times, even if grows rapidly at infinity: each trajectory samples just one fixed velocity. Its inverse is , and its Jacobian matrix is the block triangular matrix
Consequently its Jacobian determinant is one. The nonzero Jacobian determinant of is unnecessary for this construction.

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