Extremely Confusing Energy Question - Involves Springs

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A 1.5 kg steel mass is dropped from a height of 0.37 m onto a vertical compression spring with a force constant of 210 N/m. The problem involves calculating the maximum compression of the spring using energy conservation principles. The gravitational potential energy of the mass is converted into elastic potential energy of the spring, leading to the equation mg(h+x) = 1/2 kx^2. This results in a quadratic equation where the distance the mass falls is the sum of the height and the compression distance. Solving this equation will yield the maximum compression of the spring.
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I drew out a diagram for this question and wrote out all my givens. I looked through all the formula's I have and I just can't put the pieces of the puzzle together. If anyone can help that would be greatly appreciated.

Question:

A 1.5kg steel mass is dropped onto a vertical compression spring of force constant 2.1 x 10^2 N/m, from a height of 0.37m above the top of the spring. Find, from energy considerations, the maximum distance the spring is compressed.

Thanks!
 
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Work is the integral of force over distance.

The spring applies a force equal to F = kx. The work done in compression is the integral of that force over distance:

W = integral (from 0 to p) (k x dx)
= 1/2 k x^2 | p
= 1/2 k p^2

where p is the maximum compression distance.

Find the gravitational potential energy released by a 1.5 kg mass moving 0.37m downwards (it's just [delta]E = m g y). Set it equal to the work done in the spring's compression, and solve for p.

- Warren
 
I'm guessing that this is not a calculus-based class, is it?

Without calculus it's the same as Chroot said, but it looks a little different. Use conservation of energy, the gravitational potential energy at height "h" above the spring equals the total elastic potential energy of the spring when compressed a distance "x." The trick here is that the distance the mass falls is "h+x." THis is going to lead you to a quadratic solution.
mg(h+x) = 1/2 kx^2.
 
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