The object’s position as a function of time is
"x(0)=0\\to \\phi=\\pm \\frac{\\pi}{2}"
Since the object is traveling to the right, it is in the lower half of the circular motion diagram, giving a phase constant between "-\\pi" and 0 radians. Thus,
"\\omega=\\frac{2\\pi}{T}=\\frac{2\\pi}{4}=\\frac{\\pi}{2}\\frac{rad}{s}"
"x=A\\cos(\\frac{\\pi}{2}t-\\frac{\\pi}{2})=A\\sin{\\frac{\\pi}{2}t}"
So,
"t=0.28\\ s"
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