(a) By Eq. $$ \ V_f-V_i=- \int^f_i \overset{\rightarrow}{E}.\overset{\rightarrow}{ds}$$, the change in potential is the negative of the "area" under the curve. Thus, using the area-of-a-triangle formula, we have
$$ V-10=- \int^{x=2}_0 \overset{\rightarrow}{E}.\overset{\rightarrow}{ds} = \dfrac{1}{2} (2)(20)$$
which yields $$V=30 \ V$$
(b) For any region within $$0<x<3m, - \int \overset{\rightarrow}{E}.\overset{\rightarrow}{ds}$$ is positive, but for any region for which $$x>3 \ m$$ it is negative. Therefore, $$V=V_{max}$$ occurs at $$x=3 \ m$$
$$ V-10=- \int^{x=3}_0 \overset{\rightarrow}{E}.\overset{\rightarrow}{ds} = \dfrac{1}{2} (3)(20) $$
which yields $$V_{max} = 40 \ V$$.
(c) In view of our result in part (b), we see that now (to find $$V=0$$) we are looking for some $$X>3 \ m$$ such that the "area" from $$x=3 \ m$$ to $$x=X$$ is $$40 \ V$$. Using the formula for a triangle $$(3<x<4)$$ and a rectangle $$(4<x<X)$$, we require
$$ \dfrac{1}{2}(1)(20) + (X-4)(20) = 40 $$
Therefore, $$X=5.5 \ m$$.