Without loss of generality, let us assume that at time t = 0 an oscillator passes the equilibrium position (x = 0). Hence, its law of motion has the following form:
"x(t) = A \\sin{\\omega t}" We observe the considered positions (A/2 and A) of the oscillator at the moments of time:
"x(t_1) = \\frac{A}{2} = A \\sin{\\omega t_1} \\, \\Rightarrow \\, \\sin{\\omega t_1} = \\frac{1}{2} \\, \\Rightarrow \\, \\omega t_1 = \\frac{\\pi}{6}" and
"x (t_A) =A = A \\sin{\\omega t_A} \\, \\Rightarrow \\, \\sin{\\omega t_A} = 1 \\, \\Rightarrow \\, \\omega t_A = \\frac{\\pi}{2}" The time t2 is just the difference between tA and t1:
"t_2 = t_A - t_1 \\, \\Rightarrow \\, \\omega t_2 = \\omega t_A - \\omega t_1 = \\frac{\\pi}{3}" Finally,
"\\frac{t_2}{t_1} = \\frac{\\omega t_2}{\\omega t_1} = \\frac{\\pi\/3}{\\pi\/6} = 2" Answer: the ratio between t2 and t1 is 2.
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