Surface integrals are used for computations of
- surface area;
- volume of a solid enclosed by a surface.
Consider these applications in more details.
Surface Area
Suppose \(S\) be a smooth piecewise surface. The area of the surface is given by the integral
\[A = \iint\limits_S {dS} .\]
If the surface \(S\) is parameterized by the vector
\[\mathbf{r}\left( {u,v} \right) = x\left( {u,v} \right)\mathbf{i} + y\left( {u,v} \right)\mathbf{j} + z\left( {u,v} \right)\mathbf{k},\]
then the surface area is
\[A = \iint\limits_{D\left( {u,v} \right)} {\left| {\frac{{\partial \mathbf{r}}}{{\partial u}} \times \frac{{\partial \mathbf{r}}}{{\partial v}}} \right|dudv},\]
where \({D\left( {u,v} \right)}\) is the domain where the surface is defined.
If \(S\) is given explicitly by the function \({z\left( {x,y} \right)},\) the surface area is
\[A = \iint\limits_{D\left( {x,y} \right)} {\sqrt {1 + {{\left( {\frac{{\partial z}}{{\partial x}}} \right)}^2} + {{\left( {\frac{{\partial z}}{{\partial y}}} \right)}^2}} dxdy},\]
where \({D\left( {x,y} \right)}\) is the projection of the surface \(S\) onto the \(xy\)-plane.
Volume of a Solid Bounded by a Closed Surface
Suppose that a solid is bounded by a smooth closed surface \(S.\) Then the volume of the solid is given by
\[V = \frac{1}{3}\left| {\iint\limits_S {xdydz + ydxdz + zdxdy} } \right|.\]
Solved Problems
Click or tap a problem to see the solution.
Example 1
Compute the surface area of the portion of the paraboloid \[z = 25 - {x^2} - {y^2}\] lying above the \(xy\)-plane.
Example 2
Find the area of a hemisphere of radius \(R.\)
Example 1.
Compute the surface area of the portion of the paraboloid \[z = 25 - {x^2} - {y^2}\] lying above the \(xy\)-plane.
Solution.
The surface area is given by
\[A = \iint\limits_S {dS} = \iint\limits_{D\left( {x,y} \right)} {\sqrt {1 + {{\left( {\frac{{\partial z}}{{\partial x}}} \right)}^2} + {{\left( {\frac{{\partial z}}{{\partial y}}} \right)}^2}} dxdy}.\]
Here we have
\[\frac{{\partial z}}{{\partial x}} = \frac{{ - x}}{{\sqrt {25 - {x^2} - {y^2}} }},\;\; \frac{{\partial z}}{{\partial y}} = \frac{{ - y}}{{\sqrt {25 - {x^2} - {y^2}} }}.\]
Consequently,
\[A = \iint\limits_{D\left( {x,y} \right)} {\frac{{5dxdy}}{{\sqrt {25 - {x^2} - {y^2}} }}} .\]
By changing to polar coordinates, we have
\[A = \int\limits_0^{2\pi } {d\varphi } \int\limits_0^5 {\frac{{5rdr}}{{\sqrt {25 - {r^2}} }}} = 10\pi \int\limits_0^5 {\frac{{rdr}}{{\sqrt {25 - {r^2}} }}} = - 5\pi \int\limits_0^5 {\frac{{d\left( {25 - {r^2}} \right)}}{{\sqrt {25 - {r^2}} }}} = - 5\pi \left[ {\left. {\left( {\frac{{\sqrt {25 - {r^2}} }}{{\frac{1}{2}}}} \right)} \right|_0^5} \right] = 50\pi .\]
Example 2.
Find the area of a hemisphere of radius \(R.\)
Solution.
Using the spherical coordinate system, we can describe the surface of the upper hemisphere as
\[\mathbf{r}\left( {\psi ,\theta } \right) = R\cos \psi \sin \theta \cdot \mathbf{i} + R\sin \psi \sin \theta \cdot \mathbf{j} + R\cos \theta \cdot \mathbf{k},\]
where \(0 \le \psi \le 2\pi ,\) \(0 \le \theta \le {\frac{\pi }{2}}\) (Figure \(1\)).
Figure 1.
Calculate the area element.
\[\frac{{\partial \mathbf{r}}}{{\partial \psi }}
= \frac{\partial }{{\partial \psi }}\left( {R\cos \psi \sin \theta ,R\sin \psi \sin \theta ,R\cos \theta } \right)
= \left( { - R\sin \psi \sin \theta ,R\cos \psi \sin \theta ,0} \right);\]
\[\frac{{\partial \mathbf{r}}}{{\partial \theta }}
= \frac{\partial }{{\partial \theta }}\left( {R\cos \psi \sin \theta ,R\sin \psi \sin \theta ,R\cos \theta } \right)
= \left( {R\cos \psi \cos \theta ,R\sin \psi \cos \theta , - R\sin \theta } \right).\]
Find the cross product of the given vectors:
\[\frac{{\partial \mathbf{r}}}{{\partial \psi }} \times \frac{{\partial \mathbf{r}}}{{\partial \theta }}
= \left| {\begin{array}{*{20}{c}}
\mathbf{i} & \mathbf{j} & \mathbf{k}\\
{ - R\sin \psi \sin \theta } & {R\cos \psi \sin \theta } & 0\\
{R\cos \psi \cos \theta }&{R\sin \psi \cos \theta }&{ - R\sin \theta }
\end{array}} \right|
= - {R^2}\cos \psi \,{\sin ^2}\theta \cdot \mathbf{i}
- {R^2}\sin\psi \,{\sin ^2}\theta \cdot \mathbf{j}
- {R^2}\left( {{\sin^2}\psi \sin \theta \cos \theta + {{\cos }^2}\psi \sin \theta \cos \theta } \right) \cdot \mathbf{k}
= - {R^2}\cos \psi \,{\sin ^2}\theta \cdot \mathbf{i}
- {R^2}\sin\psi \,{\sin ^2}\theta \cdot \mathbf{j}
- {R^2}\sin \theta \cos \theta \cdot \mathbf{k}.\]
Hence, the area element is
\[dS = \left| {\frac{{\partial \mathbf{r}}}{{\partial \psi }} \times \frac{{\partial \mathbf{r}}}{{\partial \theta }}} \right|d\psi d\theta
= {R^2}\sqrt {{{\sin }^4}\theta \left( {{{\cos }^2}\psi + {{\sin }^2}\psi } \right) + {{\sin }^2}\theta \,{{\cos }^2}\theta } \,d\psi d\theta
= {R^2}\sin \theta \sqrt {{{\sin }^2}\theta + {{\cos }^2}\theta } \,d\psi d\theta
= {R^2}\sin \theta \,d\psi d\theta .\]
Then the surface area of the hemisphere is given by
\[A = \iint\limits_S {dS} = \int\limits_{D\left( {\psi ,\theta } \right)} {{R^2}\sin \theta d\psi d\theta } = {R^2}\int\limits_0^{2\pi } {d\psi } \int\limits_0^{\frac{\pi }{2}} {\sin \theta d\theta } = 2\pi {R^2} \cdot \left[ {\left. {\left( { - \cos \theta } \right)} \right|_0^{\frac{\pi }{2}}} \right] = 2\pi {R^2}\left( { - \cos \frac{\pi }{2} + \cos 0} \right) = 2\pi {R^2}.\]
