The object’s position as a function of time is
x=Acos(ωt+ϕ)
x(0)=0→ϕ=±2π Since the object is traveling to the right, it is in the lower half of the circular motion diagram, giving a phase constant between −π and 0 radians. Thus,
ϕ=−2π
ω=T2π=42π=2πsrad
x=Acos(2πt−2π)=Asin2πt So,
0.059=0.14sin2πt
t=0.28 s
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