Gravitational/Spring Potential Energy problem

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pelmel92
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Homework Statement



A block of mass m starts from rest at a height h and slides down a frictionless plane inclined at angle θ with the horizontal, as shown below. The block strikes a spring of force constant k. Find the distance the spring is compressed when the block momentarily stops. (Let the distance the block slides before striking the spring be . Use the following as necessary: m, θ, k, , and g.)


Homework Equations



PE_spring = .5kx^2
PE_grav = mgh

The Attempt at a Solution



Setting the two above equations equal to each other and solving for x doesn't work... tries so far: √(2mg/k), √(-2mg/k), and one where i tried to account for the extra change in height past the natural length of the spring where i got
x=(-mgsin(ø)+√((mgsin(ø))^2 -2kmgh))/k
 
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haha whoops, i copied that over without the h's, but the answer comes up wrong even as √(2mgh/h) or √(-2mgh/k)
 
ah … without seeing the diagram, i thought the the spring was horizontal, but now i realize it's on the slope! :rolleyes:

now i understand your x=(-mgsin(ø)+√((mgsin(ø))^2 -2kmgh))/k ! :redface:

i think you have a sign wrong :wink:
 
thanks for giving me a hand :) do you mean i should subtract the square root instead of add? or should i have originally set .5kx^2 equal to -mg∆h? I'm a little confused as to how to handle this problem :/
 
well i started off with .5kx^2=mg∆H
but since the question defined h as the height the object fell when it first touches the uncompressed spring, i thought i would probably need to consider that in my ∆H.
so from there P.E.=mg(h+xsin(ø))=.5kx^2
then in quad format:
0=.5kx^2 - mgsin(ø)x -mgh