Show that the area of the inside region of a simple closed curve in the plane along the curve shortening flow is given by \begin{equation*} A(\tau) = -2\pi\tau + A(\tau = 0) \end{equation*}
As a hint, I'm supposed to first show the (more general) formula for the area; \begin{equation*} A = -\frac{1}{2} \int_\gamma \left( \gamma_\tau \cdot N_{\gamma_\tau} \right) \|\dot{\gamma}_\tau \| \text{d}t \end{equation*}
I know it has to do with using Green's theorem (Green's identity?); \begin{equation} \int_\gamma \left( \frac{\partial g}{\partial x}-\frac{\partial f}{\partial y} \right) dxdy = \int_\gamma f(x,y)dx + g(x,y)dy \end{equation} (As it appears in the book I'm following). I have a pretty clear outline of where to go after the above result (the area by integration), but I'm unsure how to get started using Green's Theorem and the Curve-Shortening Flow identities.