On the straight path , , both fields restrict to . Dotting with gives
For , the velocity is . Because throughout this path, both fields again agree pointwise, now as . Thus
These equal values alone do not establish path independence for either field on all of space.
Direct differentiation gives with , so is a conservative vector field and its integral depends only on the endpoints. In contrast,
is nonzero, for example at . Thus is not conservative. Both earlier paths lie in the surface , where the two fields happen to coincide. This illustrates why coinciding path integrals need not imply a conservative field.

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