Suppose $G$ is a finite group, and $V$ is a $\mathbb C G$-module. We can equip $V\otimes V$ with the structure of a $\mathbb C G$-module via $$g(v\otimes w) = gv\otimes gw.$$ I am trying to understand how this defines a $\mathbb C G$-module structure on the symmetric power $Sym^2(V)$ and the exterior power $\Lambda^2(V)$ as subrepresentations of $V\otimes V$ (Fulton & Harris, p.4).
I was trying to show that the action of any $g\in G$ on $(v\otimes w - w\otimes v)$ and on $(v\otimes v)$ always gives $0$, in which case, the action of $G$ induces an action on $Sym^2(V)$ and $\Lambda^2(G)$, respectively. However, I don't see why this should be true. I am also not sure why representations of these quotient of $V\otimes V$ would be "sub"-representations.