Answer:
The energy stored in the later case is equal to the energy stored in the former case of the spring.
Explanation:
For a spring we have the expression of kinetic energy as:
[tex]\rm KE=\frac{1}{2} k.x^2[/tex]
where:
k= elastic constant of the spring
x= length of deflection of the spring from the mean position
Here we are given two cases:
CASE:1
x=d
[tex]\therefore KE_1=\frac{1}{2} k.(d)^2[/tex]
CASE:2
x=-d
[tex]\therefore KE_2=\frac{1}{2} k.(-d)^2[/tex]
[tex]\therefore KE_2=\frac{1}{2} k.d^2[/tex]
So, we get
[tex]KE_1=KE_2[/tex]
Just the difference in the two cases is that there is deflection of the spring in the opposite direction.