First you need to recognize the parts of this scenario. I would draw a diagram showing the spring compressed as condition 1, condition 2 is the spring relaxed and the block moving with a speed of vlaunched, then condition 3 is a moment before the collision where the 100 g mass has the same speed vlaunched and the 300 g mass has a speed of 0 m/s, condition 4 has both blocks stuck together with a speed of vfinal.
- Part A: This is a traditional energy conservation situation, where elastic potential energy is transformed into kinetic energy of the block. You can find the elastic potential energy of condition 1 with the spring constant and compression amount (make sure to convert from cm to m) and then equate that to the kinetic energy, which you can use to solve for the vlaunched at condition 2 requested in part a using the 100 g mass (convert this to kg).
- Part B: There is a collision and all collisions should start with analyzing conservation of momentum. The only object with momentum before the collision is the 100 g mass, so determine the initial momentum based on the 100 g mass and the vlaunched. Set that equal to the momentum of the combined masses times the vfinal you will be solving for in part b.
- Part C: during any collision both objects experience equal and opposite impulse found by FΔt = Δp. You can find the change of momentum of the 100 g block easily enough (you have the mass and both vlaunched and vfinal), which will be the Δp in the equation and the t is given, so solve for F.
- Part D: requires you to find the loss in kinetic energy, which always happens in an inelastic collision, and use that as the thermal energy added to the bismuth. Find the amount of energy by calculating the initial kinetic energy (only the 100 g mass is moving - make sure to use the mass in kg) and then kinetic energy after (just add the 2 masses in kg and use the vfinal). The difference is the energy lost to thermal energy, which will be the Q in Q=mcΔT and you can solve for ΔT.