Question #26998

A bus is moving downhill at a slope of 5° on a rainy day. At the moment when the speed of the bus is
30 km h−1,the driver spots a deer 30 m ahead. He applies the brakes and comes to a stop. The deer is
paralyzed by fear and does not move. Will the bus stop before reaching it or will it hit the deer? Do
relevant calculations and draw appropriate force diagram. Take the coefficient of kinetic friction to
be μk = 0.26

Expert's answer

QUESTION:

A bus is moving downhill at a slope of 55{}^{\circ} on a rainy day. At the moment when the speed of the bus is 30km h130\mathrm{km~h - 1} (8.33 m/s), the driver spots a deer 30m30\mathrm{m} ahead. He applies the brakes and comes to a stop. The deer is paralyzed by fear and does not move. Will the bus stop before reaching it or will it hit the deer? Do relevant calculations and draw appropriate force diagram. Take the coefficient of kinetic friction to be μk=0.26\mu k = 0.26

SOLUTION:

There are three forces, acting on a bus: normal force FN\vec{F}_N, the force of friction Ffr\vec{F}_{fr} and the gravitational force mgm\vec{g}:



According to the Newton's second law of motion:


F=ma\vec {F} = m \vec {a}F=FN+mg+Ffr\vec {F} = \vec {F} _ {N} + m \vec {g} + \vec {F} _ {f r}


Hence:


{Ffr+mgsin(5o)=ma (the projection onto x axis)FNmgcos(5o)=0 (the projection onto y axis)Ffr=μFN (Amonton’s law of friction)\left\{ \begin{array}{l} - F _ {f r} + m g \sin (5 ^ {o}) = m a \text{ (the projection onto } x \text{ axis)} \\ F _ {N} - m g \cos (5 ^ {o}) = 0 \text{ (the projection onto } y \text{ axis)} \\ F _ {f r} = \mu F _ {N} \text{ (Amonton's law of friction)} \end{array} \right.{Ffr+mgsin(5o)=maFN=mgcos(5o)Ffr=μmgcos(5o){μmgcos(5o)+mgsin(5o)=maFN=mgcos(5o)Ffr=μmgcos(5o)\left\{ \begin{array}{l} - F _ {f r} + m g \sin (5 ^ {o}) = m a \\ F _ {N} = m g \cos (5 ^ {o}) \\ F _ {f r} = \mu m g \cos (5 ^ {o}) \end{array} \right. \Rightarrow \left\{ \begin{array}{l} - \mu m g \cos (5 ^ {o}) + m g \sin (5 ^ {o}) = m a \\ F _ {N} = m g \cos (5 ^ {o}) \\ F _ {f r} = \mu m g \cos (5 ^ {o}) \end{array} \right. \Rightarrow{mg(sin(5o)μcos(5o))=maFN=mgcos(5o)Ffr=μmgcos(5o)a=g(μcos(5o)sin(5o))\Rightarrow \left\{ \begin{array}{l} m g (\sin (5 ^ {o}) - \mu \cos (5 ^ {o})) = m a \\ F _ {N} = m g \cos (5 ^ {o}) \\ F _ {f r} = \mu m g \cos (5 ^ {o}) \end{array} \right. \Rightarrow a = - g \left(\mu \cos (5 ^ {o}) - \sin (5 ^ {o})\right)


The projection onto xx axis of the acceleration of the bus is negative, because the bus decelerates. Hence, the bus travels:


s=v0t+at22. Where v=v0+ats = v _ {0} t + \frac {a t ^ {2}}{2}. \text{ Where } v = v _ {0} + a t


When the bus stops,


v=0v = 00=v0+at0 = v _ {0} + a tt=v0a=v0g(μcos(5o)sin(5o))t = \frac {- v _ {0}}{a} = \frac {v _ {0}}{g (\mu \cos (5 ^ {o}) - \sin (5 ^ {o}))}


Hence


s=v0t+at22=v0v0g(μcos(5o)sin(5o))(g(μcos(5o)sin(5o)))(v0g(μcos(5o)sin(5o)))22==v02g(μcos(5o)sin(5o))v022g(μcos(5o)sin(5o))s=v022g(μcos(5o)sin(5o))s=20.6m\begin{array}{l} s = v _ {0} t + \frac {a t ^ {2}}{2} = v _ {0} \cdot \frac {v _ {0}}{g (\mu \cos (5 ^ {o}) - \sin (5 ^ {o}))} - \frac {\left(g (\mu \cos (5 ^ {o}) - \sin (5 ^ {o}))\right) \cdot \left(\frac {v _ {0}}{g (\mu \cos (5 ^ {o}) - \sin (5 ^ {o}))}\right) ^ {2}}{2} = \\ = \frac {v _ {0} ^ {2}}{g (\mu \cos (5 ^ {o}) - \sin (5 ^ {o}))} - \frac {v _ {0} ^ {2}}{2 \cdot g (\mu \cos (5 ^ {o}) - \sin (5 ^ {o}))} \\ s = \frac {v _ {0} ^ {2}}{2 \cdot g (\mu \cos (5 ^ {o}) - \sin (5 ^ {o}))} \\ s = 20.6 \, \text{m} \end{array}


This answer we can easily obtain without using the Newton's law of motion. According to the work-energy theorem


W=Ek2Ek1+Ep2Ep1W = E _ {k 2} - E _ {k 1} + E _ {p 2} - E _ {p 1}Ek2=0E _ {k 2} = 0Ek1=mv022E _ {k 1} = \frac {m v _ {0} ^ {2}}{2}Ep2Ep1=mghE _ {p 2} - E _ {p 1} = - m g hh=ssin(5o)h = s \cdot \sin (5 ^ {o})W=Ffrscos(180o)=FfrsW = F _ {f r} \cdot s \cdot \cos (180 ^ {o}) = - F _ {f r} sFfr=μFN=μmgcos(5o)F _ {f r} = \mu F _ {N} = \mu m g \cos (5 ^ {o})


Hence


μmgcos(5o)s=mv022mgssin(5o)mgssin(5o)+μmgcos(5o)s=mv022s(gsin(5o)+μgcos(5o))=v022s=v022g(μcos(5o)sin(5o))s=20.6m\begin{array}{l} - \mu m g \cos (5 ^ {o}) \cdot s = - \frac {m v _ {0} ^ {2}}{2} - m g \cdot s \cdot \sin (5 ^ {o}) \\ - m g \cdot s \cdot \sin (5 ^ {o}) + \mu m g \cos (5 ^ {o}) \cdot s = \frac {m v _ {0} ^ {2}}{2} \\ s (- g \cdot \sin (5 ^ {o}) + \mu g \cos (5 ^ {o})) = \frac {v _ {0} ^ {2}}{2} \\ s = \frac {v _ {0} ^ {2}}{2 g (\mu \cos (5 ^ {o}) - \sin (5 ^ {o}))} \\ s = 20.6 \, \text{m} \end{array}


**ANSWER:**

But will travel 20.6 meters, and won't hit a deer.


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