As tiny-tim says, the simplest thing to do is to use Gauss' theorem and integrate over the volume instead. If you want to do it directly, write the cone in parametric equations, x= r cos(\theta), y= r sin(\theta), z= r.
Now we can write each point as the vector \rho(r,\theta)= r cos(\theta)\vec{i}+ r sin(\theta)\vec{j}+ r\vec{k}.
The derivatives, \rho_r= cos(\theta)\vec{i}+ sin(\theta)\vec{j}+ \vec{k} and \rho_\theta= -r sin(\theta)\vec{i}+ r cos(\theta)\vec{j} are in the tangent plane at each point and the cross product of the two vectors, r cos(\theta)\vec{i}+ r sin(\theta)\vec{j}+ r\vec{k} is normal to the surface. The "vector differential of surface area" is d\vec{S}= (r cos(\theta)\vec{i}+ r sin(\theta)\vec{j}+ r\vec{k})drd\theta).
(I chose the order of cross product to give a negative z component so the vector is oriented downward since the problem said "down through the surface".)
Since the vector function is \vec{i}+ \vec{j}+ \vec{k} the flux is given by \int\int (\vec{i}+ \vec{j}+ \vec{k})\cdot(r cos(\theta)\vec{i}+ r sin(\theta)\vec{j}+ r\vec{k})drd\theta)) or
\int_{\theta= 0}^{2\pi}\int_{r= 1}^2 r( cos(\theta)+ sin(\theta)+ 1) drd\theta
(\theta runs from 0 to 2\pi to go all the way around the cone and r runs from 1 to 2 because z= r and we are told that "1< z< 2".)