A particle mass m is attached to two identical springs each of spring constant k and natural length a. One spring is attached at its other end to a fixed point A, the other spring to a fixed point B such that A is a height 4a vertically above B. The particle can move in the vertical line AB. If mg/2
|dw:1376218605698:dw| |dw:1376218791995:dw| I assume that my 2nd spring is still stretched upwards so the free body diagram looks like this: |dw:1376219098008:dw| They're in equilibrium so Newton's second law: \[k(x+a)=mg+k(a-x) \rightarrow x=\frac{ mg }{ 2k}\] independent of a. This is the case when force due to 2nd spring is downwards. And this is possible when \[k(a-x)>0 \rightarrow x<a\] To prove that we know \[\frac{ mg }{ 2}<ka\] and\[\frac{ mg }{ 2 }=kx\]so \[kx<ka \rightarrow x<a\] In addition (it's not the part of the answer) I'd like to see what's going to happen when x=a and x>0. In first case this is only true when \[a=x=\frac{ mg }{ 2k }\] where a is length of spring if \[x>a\] \[k(2a+x)+kx=mg \rightarrow x=\frac{ mg }{ 2k }-a\]
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