I think of Newton's First Law as a definition of an inertial frame (an inertial frame is one in which an object with no net force moves with a constant velocity) and a statement that one must be in an inertial frame to apply Newton's Laws.
Therefore, for question (a), the person inside the truck should first test whether they are in an inertial frame: place a ball on the ground; it evidently has zero net force applied to it, but it will be seen to accelerate toward the back of the truck. This "ghost force" indicates that the person is not in an intertial frame and should therefore not attempt to use Newton's Second Law.
The person standing outside the truck is in an inertial frame (they too can do an "inertial frame test" and find, to within the precision of their measurements, the ground on Earth is inertial), so they are free to apply Newton's Second Law. They must however choose a coordinate system rooted to their frame, so the acceleration of the block will be expressed as the second time derivative of the vector sum of the positions $\vec{R}$ and $\vec{r}$, where $\vec{R}$ is the (horizontal) position vector of the truck with respect to the ground and $\vec{r}$ is the usual position of the block relative to the top of the incline.
This question considers the special case that the block does not move with respect to the incline. Whether the block slides down the incline, up the incline, or does not slide at all, depends on the specifics of the problem (the acceleration of the truck and the angle of the incline).
So, for questions (b) and (d), the answer is no they will not agree. The observer on the ground will say that the acceleration of the block is approximately the same as the truck while the observer in the truck might see any kind of accleration along the incline. The horizontal distance covered from the perspective of the observer on the ground is again very similar to that covered by the truck, while for the observer in the truck it could be many things.
For question (c), the block might never reach the bottom of the incline (or might fall off the top!). But any timing of events will be the same for the two observers (in a non-relativistic situation).