The equation of the sphere of radius r, x2+ y2+ z2= R2 can be thought of as a "level surface" of the function f(x,y,z)= x2+ y2+ z2. Its gradient, grad f= 2xi+ 2yj+ 2zk is perpendicular to that surface. "Normalizing" to integrate on the xy-axis by dividing through by z2, the differential of surface area is the length of the vector (x/z)i+ (y/z)j+ k:
\sqrt{\frac{x^2}{z^2}+ \frac{y^2}{z^2}+ 1}dxdy= \frac{\sqrt{x^2+ y^2+ z^2}}{z}dxdy= \frac{Rdxdy}{z}.
Of course,
z= \sqrt{R^2- x^2- y^2}
so the integral for surface area, in polar coordinates would be
R\int \frac{rdrd\theta}{\sqrt{R^2- r^2}}
The lower boundary is z= 0 which corresponds to the circle of radius R.
The upper limit is at "60 degrees north" where z= Rsin(60)= \frac{R\sqrt{3}}{2} and thus r2+ z2= r2+ 3R2/4= R2 which reduces to r= R/2. The limits of integration are 0\le \theta \le 2\pi and 0\le r \le R/2The equation of the sphere of radius r, x2+ y2+ z2= R2 can be thought of as a "level surface" of the function f(x,y,z)= x2+ y2+ z2. Its gradient, grad f= 2xi+ 2yj+ 2zk is perpendicular to that surface. "Normalizing" to integrate on the xy-axis by dividing through by z2, the differential of surface area is the length of the vector (x/z)i+ (y/z)j+ k:
\sqrt{\frac{x^2}{z^2}+ \frac{y^2}{z^2}+ 1}dxdy= \frac{\sqrt{x^2+ y^2+ z^2}}{z}dxdy= \frac{Rdxdy}{z}.
Of course,
z= \sqrt{R^2- x^2- y^2}
so the integral for surface area, in polar coordinates would be
R\int \frac{rdrd\theta}{\sqrt{R^2- r^2}}
The lower boundary is z= 0 which corresponds to the circle of radius R.
The upper limit is at "60 degrees north" where z= Rsin(60)= \frac{R\sqrt{3}}{2} and thus r2+ z2= r2+ 3R2/4= R2 which reduces to r= R/2. The limits of integration are 0\le \theta \le 2\pi and 0\le r \le R/2The equation of the sphere of radius r, x2+ y2+ z2= R2 can be thought of as a "level surface" of the function f(x,y,z)= x2+ y2+ z2. Its gradient, grad f= 2xi+ 2yj+ 2zk is perpendicular to that surface. "Normalizing" to integrate on the xy-axis by dividing through by z2, the differential of surface area is the length of the vector (x/z)i+ (y/z)j+ k:
\sqrt{\frac{x^2}{z^2}+ \frac{y^2}{z^2}+ 1}dxdy= \frac{\sqrt{x^2+ y^2+ z^2}}{z}dxdy= \frac{Rdxdy}{z}.
Of course,
z= \sqrt{R^2- x^2- y^2}
so the integral for surface area, in polar coordinates would be
R\int \frac{rdrd\theta}{\sqrt{R^2- r^2}}
The lower boundary is z= 0 which corresponds to the circle of radius R.
The upper limit is at "60 degrees north" where z= Rsin(60)= \frac{R\sqrt{3}}{2} and thus r2+ z2= r2+ 3R2/4= R2 which reduces to r= R/2. The limits of integration are 0\le \theta \le 2\pi and 0\le r \le R/2The equation of the sphere of radius r, x2+ y2+ z2= R2 can be thought of as a "level surface" of the function f(x,y,z)= x2+ y2+ z2. Its gradient, grad f= 2xi+ 2yj+ 2zk is perpendicular to that surface. "Normalizing" to integrate on the xy-axis by dividing through by z2, the differential of surface area is the length of the vector (x/z)i+ (y/z)j+ k:
\sqrt{\frac{x^2}{z^2}+ \frac{y^2}{z^2}+ 1}dxdy= \frac{\sqrt{x^2+ y^2+ z^2}}{z}dxdy= \frac{Rdxdy}{z}.
Of course,
z= \sqrt{R^2- x^2- y^2}
so the integral for surface area, in polar coordinates would be
R\int \frac{rdrd\theta}{\sqrt{R^2- r^2}}
The lower boundary is z= 0 which corresponds to the circle of radius R.
The upper limit is at "60 degrees north" where z= Rsin(60)= \frac{R\sqrt{3}}{2} and thus r2+ z2= r2+ 3R2/4= R2 which reduces to r= R/2. The limits of integration are 0\le \theta \le 2\pi and 0\le r \le R/2