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One can always resolve these vectors in two perpendicular directions,
chosen parallel and perpendicular to the present velocity vector:
F_t = m dv/dt , and
F_c = mv^2/r . , where
F_t is the component of the net force tangential to the present velocity,
and
F_c is the component of the net force perpendicular to the velocity and
directed toward the center of curvature (r); v is the instantaneous
speed.
This can always be done and is very useful. There is no exception to this
method of decomposition of F=mA.
Bob