Method 2
Differential geometry approach. This method depends on parametrizing the surface. While it is not the fun method to solve the problem, it is the core method in solving all types of surface integrals.
Let us first write the surface integral in a different form.
\(\displaystyle \iint\limits_S z \ dS = \int\int z \ |\bold{n}| \ d\theta \ dz\)
where \(\displaystyle \bold{n}\) is the normal vector.
We have a cylinder, so the best parametrization is to use the cylindrical coordinate.
\(\displaystyle x = r\cos \theta\)
\(\displaystyle y = r\sin \theta\)
\(\displaystyle z = z\)
Since the radius \(\displaystyle r = 1\), this will be reduced to:
\(\displaystyle x = \cos \theta\)
\(\displaystyle y = \sin \theta\)
\(\displaystyle z = z\)
Then, the parametrization of the surface \(\displaystyle S\) is:
\(\displaystyle \boldsymbol{ \varphi}(\theta,z) = (\cos \theta, \sin \theta, z)\)
The normal vector is just the cross product of the partial derivatives of our parametrized surface.
\(\displaystyle \bold{n} = \frac{\partial \boldsymbol{\varphi}}{\partial \theta} \times \frac{\partial \boldsymbol{\varphi}}{\partial z}\)
With a little calculation, you will find that \(\displaystyle \frac{\partial \boldsymbol{\varphi}}{\partial \theta} \times \frac{\partial \boldsymbol{\varphi}}{\partial z} = 1\)
Then
\(\displaystyle \int\int z \ |\bold{n}| \ d\theta \ dz = \int_{1}^{2}\int_{0}^{\pi} z \ |1| \ d\theta \ dz\)
\(\displaystyle = \int_{1}^{2}\pi z \ dz = \frac{3\pi}{2}\)
One more step to see
Method 3