Ken G said:
Most second-year courses do a lot of things. They probably include Lagrangians, but also more traditional Newtonian problems, perhaps involving fictitious forces. The OPer is right that the problems require more thought and more putting together the pieces, rather than just writing down the answer (conservation of energy can often be used to just write down the answer, so is usually not enough in second-year problems, but it can often be one of the pieces, depending on the problem). If it is a Lagrangian problem, then what's tricky is identifying the generalized coordinates in ways that automatically include the constraints on the system. The rest is often quite cook-booky.
I see. At my university (in Argentina) CM is a 3rd year course but since we take "only" 3 courses per semester it would correspond to a 2nd year course in the US. The recommended books are Goldstein's and Landau & Lifgarbagez's books (our programme consists almost exclusively of the name of the chapters in the latter book). We have 7 sets of assignments, number 0 (called "Before the beginning") has only Newtonian mechanics problems. The final exam counts for 100% of our mark for that course. I've never seen any Newtonian mechanics problem in past exams.
For this course at my university, knowing how include the constraint equation(s) into the potential energy part of the Lagrangian isn't enough, for a Lagrangian problem. Indeed, they can ask us to solve the problem using Lagrange multipliers and thus to write the "modified" Lagrangian. So it's not only a matter on how to transcript the problem into mathematical expression and then solve it; it's also about solving the problem in all possible ways.
Also, they ask us what quantities are conserved. We cannot say "angular momentum" without any algebra that back up this claim. We have to show that a coordinate is cyclic in the Lagrangian and therefore the generalized momentum associated to this coordinate is a constant of motion.
So unlike the first year course, you can't just assume that the angular momentum is conserved and use this fact to solve a problem. This may sound ridiculous but this is the way it is.
P.S.:1)I know a member in this forum from Spain and he described his course as very similar to mine, with the same books recommended, etc. So I don't think my university is a "special case".
2)I didn't take the final exam yet but I can take it on the 7th of March if I feel ready. I still have a mountain to study. I must reach Poisson's bracket and Hamilton-Jacobi reformulation of CM. :/ Also have to study Euler's angles and canonical transformations.
3)To answer the OP: I've noticed that this 2nd year course takes a very, very long of my (and friends) time. If you don't know how to even start a problem, try to find a similar problem in as many books on CM as you can and on the Internet. If you're stuck you can post here or ask friends/professors to help you. Do not "suffer" silently.