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Question 1
A parcel rests on the horizontal floor of a van. The van is travelling on a level road at 14 m s$^{-1}$. It is brought to rest by a uniform application of the brakes... show full transcript
Step 1
Answer
To determine if the parcel is on the point of sliding forward, we first need to find the deceleration of the van due to braking. The force of friction acting on the parcel can be expressed as:
F_f = rac{2}{5} mg
Assuming the braking force , we equate the forces:
-ma = -rac{2}{5} mg
This implies:
a = rac{2}{5} g
Using the equation of motion to find the stopping distance:
Setting the final velocity and initial velocity :
0 = (14)^2 + 2igg(-rac{2}{5}gigg)s
Solving for gives:
0 = 196 - rac{4g}{5}s rac{4g}{5}s = 196 s = rac{5 imes 196}{4g}
Calculating for gives:
s = rac{5 imes 196}{39.24} \ \\ s \approx 25 ext{ m}
Therefore, the parcel is indeed on the verge of sliding forward.
Step 2
Answer
To show the above relationship, we need to analyze the movement of both cars. For car C:
It accelerates with an acceleration eta from rest to maximum speed . The distance covered during this acceleration is:
d_C = rac{1}{2} eta t^2
After reaching speed , it travels at constant speed for the remaining distance.
For car D:
It moves at a constant speed rac{3u}{4}. Over the time it covers:
d_D = rac{3u}{4} t
Setting , we find:
rac{1}{2} eta t^2 = rac{3u}{4} t \\ \\ ext{Solving for } t:\ \ eta t=rac{3u}{2} o t = rac{3u}{2eta}
Next, car C travels for time t_2 = rac{4d}{3u} - rac{d}{eta}, rearranging and substitute:
d = rac{1}{2}eta t_2^2 + ut_2
Substituting in reference to time relationships gives the expression showing they are related.
Step 3
Answer
Using the results from the acceleration and constant speed journeys:
For car C:
For the distance travelled during acceleration phase:
d_1 = rac{1}{2} eta t_1^2
Total distance when reaching speed and travelling in constant speed afterwards:
d = rac{1}{2}eta igg(rac{u}{eta}igg)^2 + ut_2
Where:
ext{Combine these to solve: } d = rac{u^2}{2eta} + uigg(rac{4d}{3u} - rac{d}{eta}igg)
Simplifying gives:
d = rac{3u^2}{2eta}
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