(a) 5.35 s, 84.65 s
The distance covered by the rocket during the first part of the motion (accelerated motion) is
(1)
where
a = +35 ft/s^2 is the acceleration
While the distance covered during the second part of the motion (uniform motion) is
where v is the constant speed reached after the first part of the motion, which is given by
![v=at_1](https://tex.z-dn.net/?f=v%3Dat_1)
So we can rewrite the equation as
(2)
We also know:
(3) is the total distance
(4) is the total time
We can rewrite (3) as
(5)
And (4) as
![t_2 = 90-t_1](https://tex.z-dn.net/?f=t_2%20%3D%2090-t_1)
Substituting into (5), we get
![\frac{1}{2}at_1^2 + a t_1 (90-t_1) = 16350\\0.5 at_1^2 + 90at_1 - at_1^2 = 16350\\-0.5at_1^2 +90at_1 = 16350](https://tex.z-dn.net/?f=%5Cfrac%7B1%7D%7B2%7Dat_1%5E2%20%2B%20a%20t_1%20%2890-t_1%29%20%3D%2016350%5C%5C0.5%20at_1%5E2%20%2B%2090at_1%20-%20at_1%5E2%20%3D%2016350%5C%5C-0.5at_1%5E2%20%2B90at_1%20%3D%2016350)
Substituting a=+35 ft/s^2, we have
![-17.5 t_1^2 +3150 t_1 - 16350 = 0](https://tex.z-dn.net/?f=-17.5%20t_1%5E2%20%2B3150%20t_1%20-%2016350%20%3D%200)
which has two solutions:
--> discarded, since the total time cannot be greater than 90 s
--> this is the correct solution
And therefore
is
![t_2 = 90-t_1 = 90 -5.35 s=84.65 s](https://tex.z-dn.net/?f=t_2%20%3D%2090-t_1%20%3D%2090%20-5.35%20s%3D84.65%20s)
(b) 187.25 ft/s
The velocity v is the velocity at the end of the accelerated motion of the rocket, so after
![t_1 = 5.35 s](https://tex.z-dn.net/?f=t_1%20%3D%205.35%20s)
The acceleration is
a = +35 ft/s^2
Therefore, the velocity after the first part is:
![v=at_1 = (+35 ft/s^2)(5.35 s)=187.25 ft/s](https://tex.z-dn.net/?f=v%3Dat_1%20%3D%20%28%2B35%20ft%2Fs%5E2%29%285.35%20s%29%3D187.25%20ft%2Fs)
(c) 16,585 ft
At the 15750 ft mark, the velocity of the sled is
![v=187.25 ft/s](https://tex.z-dn.net/?f=v%3D187.25%20ft%2Fs)
Then, it starts decelerating with acceleration
a = -21 ft/s^2
So, its distance covered during this part of the motion will be given by:
![v_f ^ 2 -v^2 = 2ad_3](https://tex.z-dn.net/?f=v_f%20%5E%202%20-v%5E2%20%3D%202ad_3)
where
vf = 0 is the final speed
v = 187.25 ft/s is the initial speed
a = -21 ft/s^2 is the acceleration
d3 is the distance covered during this part
Solving for d3,
![d_3 = \frac{v_f^2 -v^2}{2a}=\frac{0-(187.25 ft/s)^2}{2(-21 ft/s^2)}=835 ft](https://tex.z-dn.net/?f=d_3%20%3D%20%5Cfrac%7Bv_f%5E2%20-v%5E2%7D%7B2a%7D%3D%5Cfrac%7B0-%28187.25%20ft%2Fs%29%5E2%7D%7B2%28-21%20ft%2Fs%5E2%29%7D%3D835%20ft)
So, the final position of the sled will be
![x_3 = 15750 ft + 835 ft =16,585 ft](https://tex.z-dn.net/?f=x_3%20%3D%2015750%20ft%20%2B%20835%20ft%20%3D16%2C585%20ft)
(d) 93.92 s
The duration of the first part of the motion is
![t_1 = 5.35 s](https://tex.z-dn.net/?f=t_1%20%3D%205.35%20s)
The distance covered during this part is
![d_1 = \frac{1}{2}at_1^2=\frac{1}{2}(+35 ft/s^2)(5.35 s)^2=501 ft](https://tex.z-dn.net/?f=d_1%20%3D%20%5Cfrac%7B1%7D%7B2%7Dat_1%5E2%3D%5Cfrac%7B1%7D%7B2%7D%28%2B35%20ft%2Fs%5E2%29%285.35%20s%29%5E2%3D501%20ft)
In the second part (uniform motion), the sled continues with constant speed until the 15750 ft mark, so the distance covered is
![d_2 = 15750- 835 =14915](https://tex.z-dn.net/?f=d_2%20%3D%2015750-%20835%20%3D14915)
And so the duration of the second part is
![t_2 =\frac{d_2}{v}=\frac{14915}{187.25}=79.65 s](https://tex.z-dn.net/?f=t_2%20%3D%5Cfrac%7Bd_2%7D%7Bv%7D%3D%5Cfrac%7B14915%7D%7B187.25%7D%3D79.65%20s)
While the duration of the third part (decelerated motion) is
![a=\frac{v_f-v}{t_3}\\t_3 = \frac{v_f-f}{a}=\frac{0-(187.25 ft/s)}{-21 ft/s^2}=8.92 s](https://tex.z-dn.net/?f=a%3D%5Cfrac%7Bv_f-v%7D%7Bt_3%7D%5C%5Ct_3%20%3D%20%5Cfrac%7Bv_f-f%7D%7Ba%7D%3D%5Cfrac%7B0-%28187.25%20ft%2Fs%29%7D%7B-21%20ft%2Fs%5E2%7D%3D8.92%20s)
So the total duration is
t = 5.35 s+79.65 s+8.92 s=93.92 s