Not sure where i went wrong

  • Thread starter mullets1200
  • Start date
In summary, the cable car descends a 200-m-high hill with the help of its brakes and a counterweight. The cable car and counterweight have negligible rolling friction and are on a 30-20-130 triangle. To maintain constant speed, the cable car needs a braking force of 3780 N. If the brakes fail, the speed of the runaway car at the bottom of the hill can be calculated by considering the change in kinetic energy and the heights gained and dropped on each side of the triangle.
  • #1
mullets1200
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0

Homework Statement


The 1990 kg cable car shown in the figure descends a 200-m-high hill. In addition to its brakes, the cable car controls its speed by pulling an 1780 kg counterweight up the other side of the hill. The rolling friction of both the cable car and the counterweight are negligible.

The trangle that this is on is a 30-20-130 triangle. The counter weight is on the 20 degree side while the cable car is on the 30 degree side

1) How much braking force does the cable car need to descend at constant speed?
3780 N

2) One day the brakes fail just as the cable car leaves the top on its downward journey. What is the runaway car's speed at the bottom of the hill?



The Attempt at a Solution


for part 1 i did:
1990*g*sin(30)-1780*g*sin(20)
3780N which was correct

for part 2 i did:
The height dropped on the AB side is 200m
The height gained on the BC side is
200/L=sin(30)
L=200/sin(30)
hbc*sin(30)/200=sin(20)
hbc=200*sin(20)/sin(30)
137 m

m*g*(200-137)=.5*m*v^2
v=sqrt(2*g*63)
35 m/s but it was wrong.

any help?
 
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  • #2
mullets1200 said:
m*g*(200-137)=.5*m*v^2

any help?

The cable car and the counter weigth have a different mass, so m*g*(200-137) is
wrong.
You also need to account for the increase in kinect energy of both the car and
the counterweight.
 

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