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A body of mass M, executes vertical SHM with periods t1 and t2, when separately attached to spring A and spring B respectively. The period of SHM, when the body executes SHM, as shown in the figure is t0. Then
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- t0–1 = t1–1 + t2–1
- t0 = t1 + t2
- t02 = t12 + t22
- t0–2 = t1–2 + t2–2
Correct Option: D
t = 2π | ![]() | |
k |
⇒ k = Const . t-2
Here the springs are joined in parallel. So
k0 = k1 - k2
where k0 is resultant force constant
or , Const . t0-2 = Const . t1-2 + Const . t2-2
or , t02 = t12 + t22