Answer:
[tex]d=109.2m[/tex]
Explanation:
We divide the problem in 3 parts: part 1 when the car accelerates, part 2 when its velocity is constant and part 3 when it slows down and we use the main equations for accelerated motion [tex]v=v_i+at[/tex] and [tex]d=v_it+\frac{at^2}{2}[/tex], and for the last part [tex]v^2=v_i^2+2ad[/tex]
We start calculating the displacement and final velocity of part 1 considering the initial velocity is zero:
[tex]d_1=v_{i1}t_1+\frac{a_1t_1^2}{2}=(0m/s)(6s)+\frac{(2m/s^2)(6s)^2}{2}=36m[/tex]
[tex]v_1=v_{01}+a_1t_1=(0m/s)+(2m/s^2)(6s)=12m/s[/tex]
Now we calculate the displacement of part 2 considering the velocity remains constant since acceleration is zero:
[tex]d_2=v_{i2}t_2=(12m/s)(2.1s)=25.2m[/tex]
Now we calculate the displacement of part 3 considering the initial velocity is the final velocity of the previous part and that it slows down until coming to rest:
[tex]d_3=\frac{v_3^2-v_{i3}^2}{2a_3}=\frac{(0m/s)^2-(12m/s)^2}{2(-1.5m/s^2)}=48m[/tex]
So our total displacement is [tex]d=d_1+d_2+d_3=36m+25.2m+48m=109.2m[/tex]