If the form is for a scalar function with continuous second partial derivatives, then and . Equality of the mixed partial derivatives therefore requires
This is necessary for an exact differential. For continuously differentiable coefficients on a simply connected open domain it is also sufficient; on a domain with holes, the equality alone need not give a single-valued global potential.
For the printed coefficients, and . Their cross derivatives are
They are not equal as functions; their difference is . Hence the form is not exact. Agreement on certain lines or isolated points is insufficient, because exactness requires the derivative identity throughout an open domain.
Let . Then , and the complex trigonometric identity gives
Thus the form is exact, with complex-valued scalar potential . Differentiating that potential with respect to the two real variables checks both coefficients individually.
Away from zeros of , an integrating factor for a differential one-form is . Multiplication converts the form to
Therefore the implicit solution family is . On each graph interval between consecutive multiples of , this becomes
No such open interval contains zero. At , the undivided graph equation would read , which is impossible for a finite derivative; hence no differentiable graph extends across one of these points.
If solutions are instead understood as arbitrary parametrized integral curves of the differential form, the vertical lines are additional solutions: along them and . They were lost on division by and are not graphs over an interval.
View with and . Hold fixed and apply the multivariable chain rule:
Dividing the changes along the fixed- variation by gives exactly the two terms in the question. Thus the simpler expression is
The subscripts specify which coordinate is held fixed and must be retained.

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