You're close, but I think you would benefit by drawing a diagram of what's happening so that you can visualize your energy changes when writing out your equations. For example, before Harry jumps the situation is like this:
View attachment 275881
Now clearly, Harry falls a distance (h1 - h2) before hitting the trampoline. When the trampoline has maximally stretched the situation is as follows:
View attachment 275882
As you can see, Harry falls an additional distance Δx, stretching the springs. So that's an additional mgΔx of potential energy going into system. What's the total distance that Harry falls? That gives you the total PE "sourced" and converted to other energy. Can you write an expression that describes the total gravitational PE that goes towards stretching the trampoline springs to their maximum for this situation?
How far do the springs stretch? That gives you the energy transferred to the springs, which should be equal to the "sourced" energy from gravitation.
A nit-pick: In a real-life trampoline the springs don't stretch vertically. They go from approximately horizontal to some angle below the horizontal, so the vertical deflection of the trampoline mat is something different from the actual stretching of the springs depending upon the geometry of the trampoline. It's not a trivial exercise to work out how the energy will be distributed amongst the springs for a non-circular trampoline.
For part (b) you need to find the net force acting on Harry when the trampoline is maximally stretched. If you found Δx while doing part (a) that shouldn't be a problem.
For part (c) you need to consider what losing 30% of the system energy does to the height of the bounce. If he leaves the trampoline surface with 70% of the energy he arrived with, how does that affect height he returns to? Look at how KE and gravitational PE exchange. Also note that they ask for his height above the trampoline, not the ground for this part.