Hi Ken!
The way I would attack this is by conservation of mechanical energy (mechanical energy (ME) is the sum of the kinetic energy (KE) plus the potential energy (PE) in the system at any moment). The spring force is conservative, which means that -- at any point where the spring force is the only one doing work, as is the case while firing the ball -- the mechanical energy of the ball-spring system is constant.
Let's look at the mechanical energy (MEo) right at the instant when the spring is unlocked and just begins to fire the ball. At this point, the ball is not yet moving (we are neglecting any mass in the spring for all of this, as the problem seems to want us to assume).
MEo = KEo + PEo
At this instant of beginning, there is no kinetic energy in the system because the ball (the only object with appreciable mass) is not moving (note: KE = (1/2)mv2 for an object of mass m with speed v). But the spring has potential energy, which takes the form PEs = (1/2)kx2, where k is the force constant (or spring constant) of the spring, and x is the amount it is compressed.
So, at the start, we have:
MEo = 0 + (1/2)kx2
Once the spring has fully uncoiled, and the ball is about to leave it, we have a different situation. Now, there is no compression on the spring, so x = 0. Thus, PEs = 0 at this point.
But now the ball has some departing speed, v. So, at this point, we have:
MEf = (1/2)mv2 + 0 (where m is the mass of the ball and v is its speed.
Since mechanical energy is constant through this process, ideally, we can say that
MEf = MEo
(1/2)kx2 = (1/2)mv2
One way of describing this is that all the potential energy at the beginning has been transformed to kinetic energy by the time the ball is released. We can then relate the ball's release speed to other given quantities by solving this equation for v.
v = (k/m)1/2x
This gives the departure velocity in terms of other quantities given in the problem.
The force constant is a measure of how much force it takes to stretch or compress the spring some set length. Stiffer springs take more force to stretch or compress a given length, and thus have higher force constants. The force constant is given in units of force/length... which, as presented in this problem, is pounds per inch (the pounds of force required to stretch or compress the spring by one inch). One spring has k1 = 5 lb/in, and the other has k2 = 10 lb/in.
So, for the first spring mentioned, which I label Spring 1:
k1 = 5 lb/in
x1 = 10 in
And for the second spring, Spring 2:
k2 = 10 lb/in
x2 = 5 in
(and the same alloy, same design argument takes out engineering considerations from the final result).
As is mentioned, there two situations give the same load (since F = kx, in magnitude, for a spring). But if you put them into the expression for v above, you may see that they come out with different values (given the (1/m)1/2 is the same for both cases).
I hope this helps you on your way, but if you want to check an answer, or have more questions, just let me know.
Ken H.
08/29/16