Cars colliding into each other.

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In a scenario where car A collides with car B, which then pushes B into car C, the collisions are completely inelastic. The initial kinetic energy of car A is dissipated during the collisions, and the problem requires calculating the fraction of energy lost in the collision with car C. The conservation of momentum is applied to find the velocities after each collision, leading to expressions for kinetic energy before and after the collisions. The final kinetic energy after both collisions can be determined by substituting the derived velocities into the kinetic energy formula. The fraction of energy dissipated is then calculated by comparing the initial kinetic energy to the final kinetic energy after both collisions.
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Homework Statement


Cars B and C are at rest with their brakes off. Car A plows into B at high speed, pushing B into C. Assume the collisions are completely inelastic. What fraction of the initial energy is dissipated in the collision involving car C?
Data: MA = 1010 kg; MB = 1250 kg; MC = 1470 kg.



Homework Equations


Pinitial=Pfinal
KE=.5mv^2

The Attempt at a Solution


Pi=Pf
m_a*Vo=(m_a+m_b+m_c)*Vo'
Q+.5m_aVo^2=.5(m_a+m_b+m_c)Vo'^2; where Q is the kinetic energy lost

I'm pretty sure these equations are correct but I don't know where to go from here?
 
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Treat the problem as two separate collisions. Prior to any collision, car A has all the available kinetic energy. A collides with B and they stick together and move with a new velocity with momentum is conserved. The pair then have a collision with C, resulting in another new velocity for the trio (KE final).
 
Ok, so how would I be able to find the fraction of the first one?
 
kraigandrews said:
Ok, so how would I be able to find the fraction of the first one?

Find the KE after the first collision, then the remaining KE after the second collision. The difference between these two is the KE lost in the second collision. Compare this with what you started with before any collisions.
 
Ok sorry, I'm struggling with this one. So I have:
for the first collision:
MA*Vo=(MA+MB)*Vo'
then I solved for Vo'=((MA/(MA+MB))Vo

then plugged it into:
.5MAVo^2=.5(MA+MB)Vo'^2=.5((MA^2)/(MA+MB))-Q; I assumed Vo=1
then solved for Q, but then I am unsure of:
1. if this makes any sense
2. if .5MAVo^2=Eo then going forth from here can I do the same for the second collision solving for Q2 then add them together and end up with:
(Eo-(Q+Q2))/Eo for the fraction?
 
kraigandrews said:
Ok sorry, I'm struggling with this one. So I have:
for the first collision:
MA*Vo=(MA+MB)*Vo'
then I solved for Vo'=((MA/(MA+MB))Vo

then plugged it into:
.5MAVo^2=.5(MA+MB)Vo'^2=.5((MA^2)/(MA+MB))-Q; I assumed Vo=1
then solved for Q, but then I am unsure of:
1. if this makes any sense
2. if .5MAVo^2=Eo then going forth from here can I do the same for the second collision solving for Q2 then add them together and end up with:
(Eo-(Q+Q2))/Eo for the fraction?

Kinetic energy isn't conserved in an inelastic collision. So don't try to write conservation of kinetic energy equations :smile:

You found the velocity Vo' of the car A+B tangle, and that will yield the kinetic energy of the pair as it moves towards car C. Also, there's no need to assume that Vo=1. Just keep Vo as Vo... it'll cancel out in the end when you form your ratio of energies.

The KE of cars A+B is (1/2)(MA+MB)*Vo'^2. You can plug in the expression for Vo'.

You've got Vo' and the mass of the A+B pair, so determine the final velocity after the A+B+C collision using conservation of momentum. Use that to find the expression for the final KE.
 
I'm not sure I follow because if i use consveration of momentum again ill just end up with another variable Vo'' because if i do:
(Ma+Mb)Vo'=(Ma+Mb+Mc)Vo'' it doesn't work out.
so i am confused on how to find final KE
 
The first car, A alone, starts off with some velocity Vo. It collides with and 'sticks' to car B, and together they end up with some velocity Vo' that is a calculable fraction of Vo. The pair also retains the original momentum.

This pair then collides with car C, resulting in yet another velocity, say Vo''. It will be a fraction of the the velocity Vo'. Vo' and Vo'' can therefore be written in terms of the original Vo by substitution.
 

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