I wanted to show that a force such as drag is not a conservative force but cannot apply my method of approach. Suppose we took the situation with drag at high speeds, so $\vec D=c|\vec v|\vec v$ for some $c$.
Since work is defined as $\int_C \vec F \cdot d\vec s$ along a path $C$, if I could show that this integral differs depending on the path taken, then I would have shown that drag is non-conservative.
So the integral I would have is: $\int_C -(c|\vec v|\vec v)\cdot d\vec s$ and we can write $\vec v$ as $|v|\hat{e_t}$ which is a vector in the tangential direction to the path. Since $d\vec s$ is defined as $\hat{e_t}\cdot ds$ then the integral becomes $$\int_C -(c|\vec v|\vec v)\cdot d\vec s=\int_C -(c|\vec v|^2)ds$$
How would I proceed from here?