For the one-dimensional motion, described by x = t–sint
(a) x (t) > 0 for all t > 0.
(b) v (t) > 0 for all t > 0.
(c) a (t) > 0 for all t > 0.
(d) v (t) lies between 0 and 2.
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Initially: at t= 0, x = 0 - sin 0 = 0..
Differentiate: x' = 1 - Cos t
as cos t <= 1, x' >= 0... Hence, x raises with time..
So x(t) > 0 for all t > 0..
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v(t) = x ' (t) = 1 - cos t = 0 for t = 2 n π
so v (t) > 0 is not always true
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a (t) = Sin t = 0 for t = 2n π
so a(t) is not always > 0..
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v(t) = 1 - cos t as -1 <= cos t <= 1
so 0 <= v (t) <= 2
Differentiate: x' = 1 - Cos t
as cos t <= 1, x' >= 0... Hence, x raises with time..
So x(t) > 0 for all t > 0..
============
v(t) = x ' (t) = 1 - cos t = 0 for t = 2 n π
so v (t) > 0 is not always true
===========
a (t) = Sin t = 0 for t = 2n π
so a(t) is not always > 0..
========
v(t) = 1 - cos t as -1 <= cos t <= 1
so 0 <= v (t) <= 2
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