chwala said:
Alternatively, i think we may use integration; that is,
From;
$$v=0.6t-3.6$$
$$\int_t ^{12} (0.6t-3.6) \, dt=3.6$$ Integration yields,
$$[0.3t^2-3.6t]=3.6$$ with limits from ##t_m## to ##12##. On substituting our limits we end up with;
$$[43.2-43.2]-[0.3t_m^2-3.6t_m]=3.6$$$$-0.3t_m^2+3.6t_m-3.6=0$$
from here the steps to solution would follow. In this approach, we deliberately avoided use of acceleration.
Cheers.
I have previously replied to this post, but at that time I did not realize that this was the correct for ##v(t)## on the interval, ##\displaystyle \ 2\le t\le12\,,\ ## due to the "y-intercept" being ##-3.6## while that of the velocity graph was zero.
I suppose that rather than using the slope-intercept form for the velocity, I would be inclined to use a point-slope form and state that fact. in this case we get:
##\quad \quad \displaystyle v(t)=(0.6)(t-6)## ,
which obviously is zero at ##t=6## and has a slope of ##0.6## m/s
2 . Of course this is equivalent to the velocity function that you used .
Yes, you are correct. We can use integration to find the displacement (distance and direction) of the particle. In specific, we can use integration to find the time, ##t_m## at which the particle returns to its initial position ##X##. Since you have found that at ##t=12\,##s, particle has moved past ##X## by ##3.6\,##m, we can integrate the velocity from ##t_m## to ##12\,##s to get a displacement of ##3.6\,##m, and solve for ##t_m##.
##\quad \quad \displaystyle \int_{t_m}^{12}(0.6)(t-6) dt = 3.6##
##\quad \quad \displaystyle \left. \dfrac{0.6}{2} (t-6)^2 \right |_{t_m}^{12} = 3.6 ##
##\quad \quad \displaystyle \dfrac{3}{10} \left( (12-6)^2 - (t_m-6)^2 \right )= 3.6 ##
##\quad \quad \displaystyle 36 - (t_m-6)^2 = \dfrac{10}{3}3.6 ##
##\quad \quad \displaystyle (t_m-6)^2 =36-12 =24##
So that ##\quad \displaystyle t_m=6\pm \sqrt{24\ } \approx 6\pm 4.89898 = 1.01012 \text{ or } 10.89898 ##
The smaller number is not between 2 s and 12 s .
So to the nearest 0.1 second, the answer is ##\displaystyle t_m=10.9\,##s .
.