The Cross Partial Property Of Conservative Vector Fields

Let \(\textbf{F}\) be a vector field in three dimensions such that the component functions of \(\textbf{F}\) have continuous first-order partial derivatives on the domain of \(\textbf{F}\). Suppose \(\textbf{F}\) is a conservative vector field in \(\mathbb{R}^3\):

$$ \textbf{F}(x,y) = \langle P(x,y,z), Q(x,y,z), R(x,y,z) \rangle $$

Since \(\textbf{F}\) is conservative, there is a function \(f(x,y,z)\) such that \(∇f=\textbf{F}\). Therefore, by the definition of the gradient, \(f_x=P\), \(f_y=Q\) and \(f_z=R\). By Clairaut's theorem, \(f_{xy}=f_{yx}\), \(f_{xz}=f_{zx}\) and \(f_{yz}=f_{zy}\). This means, \(f_{xy}=P_y\) and \(f_{yx}=Q_x\), and thus \(P_y=Q_x\).

This means, \(f_{xy}=P_y\) and \(f_{yx}=Q_x\), and thus \(P_y=Q_x\).

This also means \(f_{xz}=P_z\) and \(f_{zx}=R_x\), and thus \(P_z=R_x\).

Similarly, \(f_{yz}= Q_z\) and \(f_{zy}=R_y\), and thus \(Q_z=R_y\).

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