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Derivation of the Area Formula for a Region Enclosed by a Simple Closed Plane Curve 📂Geometry

Derivation of the Area Formula for a Region Enclosed by a Simple Closed Plane Curve

Formula 1

If a simple closed curve α\alpha surrounds the region RR and rotates in a counterclockwise direction, V(R)=αxdy=αydx V (R) = \int_{\alpha} x dy = - \int_{\alpha} y dx


  • V(R)V(R) represents the volume of the region RR, or in other words, the area of RR.

Proof

According to Green’s Theorem, let’s assume that a simple planar C2C^{2} closed curve C\mathcal{C}, which is piecewise smooth, encloses a bounded region R\mathcal{R} in a counterclockwise direction.

If the two functions defined in the region R\mathcal{R}, P,QP,Q, are differentiable within R\mathcal{R}, C(Pdx+Qdy)=R(QxPy)dxdy \int_{\mathcal{C}} (Pdx + Qdy) = \iint_{\mathcal{R}} (Q_{x} - P_{y}) dx dy

By Green’s Theorem, αxdy=α(0dx+xdy)=R(xx0y)dxdy=Rxxdxdy=R1dxdy=V(R) \begin{align*} \int_{\alpha} x dy =& \int_{\alpha} \left( 0 dx + x dy \right) \\ =& \iint_{R} \left( {{ \partial x } \over { \partial x }} - {{ \partial 0 } \over { \partial y }} \right) dx dy \\ =& \iint_{R} {{ \partial x } \over { \partial x }} dx dy \\ =& \iint_{R} 1 dx dy \\ =& V(R) \end{align*} Moreover, α(xdy+ydx)=R(yyxx)dxdy=0 \int_{\alpha} \left( x dy + y dx \right) = \iint_{R} \left( {{ \partial y } \over { \partial y }} - {{ \partial x } \over { \partial x }} \right) dx dy = 0 Hence, we obtain the following. V(R)=αxdy=αydx V (R) = \int_{\alpha} x dy = - \int_{\alpha} y dx


  1. Millman. (1977). Elements of Differential Geometry: p63. ↩︎