Train vs Fly: Physics A Level Puzzle Explained

In summary: Apply all this to the bug's perspective in a collision with a windshield and you see why the bug gets smushed so easily.In summary, a collision between a train and a fly is an example of an inelastic collision, where momentum is conserved but the speeds after the collision are equal. This is due to Newton's third law, where the forces from both objects are equal. However, this does not mean that the fly will stop the train, as predicted by Newton's second law. The small area of surface on the train that collides with the fly may move backwards, stops, and moves forwards again for a brief moment, but this is only true in the frame of reference of the moving train and not in the frame of reference
  • #1
themagician
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I remember back at physics A level we were posed with the question of what happens when a train hits a fly. According to Newton laws the forces are equal, and so, by this theory, the fly should stop the train. We obviously knew that this didn't happen, but it took the whole class waaay too long to understand what was going on, but it was quite fun :)

Anyone got an answer?
 
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  • #2
themagician said:
I remember back at physics A level we were posed with the question of what happens when a train hits a fly. According to Newton laws the forces are equal, and so, by this theory, the fly should stop the train. We obviously knew that this didn't happen, but it took the whole class waaay too long to understand what was going on, but it was quite fun :)

Anyone got an answer?

Welcome to the PF.

Please look up "conservation of momentum". Then you can explain it to us! :smile:
 
  • #3
The small area of surface on the train that actually collides with the fly moves backwards, stops, and moves forwards again, same as the fly, for a very brief moment.

update - moves backwards from the frame of reference of the train. My second post clarifies this.
 
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  • #4
Forces are the same, yes, but what happens when you apply the same force to a fly or a train?
 
  • #5
themagician said:
I remember back at physics A level we were posed with the question of what happens when a train hits a fly. According to Newton laws the forces are equal, and so, by this theory, the fly should stop the train. We obviously knew that this didn't happen, but it took the whole class waaay too long to understand what was going on, but it was quite fun :)

Anyone got an answer?
No, the fly does not need the train by this theory. It is a flawed conclusion from correct premises. :)
 
  • #6
rcgldr said:
The small area of surface on the train that actually collides with the fly moves backwards, stops, and moves forwards again, same as the fly, for a very brief moment.
I haven't worked that out, but I am pretty sure that is not the case. Maybe if the fly were made of steel and the train were made of Jello.
 
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  • #7
themagician said:
I remember back at physics A level we were posed with the question of what happens when a train hits a fly. According to Newton laws the forces are equal, and so, by this theory, the fly should stop the train. We obviously knew that this didn't happen, but it took the whole class waaay too long to understand what was going on, but it was quite fun :)
Anyone got an answer?
Consider the free body diagram. Draw it out for each object!
 
  • #8
rcgldr said:
The small area of surface on the train that actually collides with the fly moves backwards, stops, and moves forwards again, same as the fly, for a very brief moment.

DaleSpam said:
I haven't worked that out, but I am pretty sure that is not the case. Maybe if the fly were made of steel and the train were made of Jello.

I meant backwards with respect to the train. It would seem that there is some moment in time where the fly's body and some tiny part of the train are stopped as the fly's molecules change direction. If this is looked from a molecular perspective, then what could be considered to be the overlapped surfaces of "touching" molecules would have to come to a stop, even if the center of the train's molecules didn't come to a stop.

If the perspective is that the fly never actually touches the train, but is repelled by the electrons, then nothing on the train comes to a stop and the fly's velocity is reversed while only slowing down some of the train's molecules.
 
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  • #9
themagician said:
I remember back at physics A level we were posed with the question of what happens when a train hits a fly.
This is an example of inelastic collision. The momentum is conserved, but the speeds after the collision are equal: [itex]m_{train}v_{train}+m_{fly}v_{fly}=(m_{train}+m_{fly})v_{after} [/itex].
 
  • #10
themagician said:
According to Newton laws the forces are equal,
That is Newtons 3rd Law only.

themagician said:
and so, by this theory, the fly should stop the train.
No, that is not what Newtons 2nd Law predicts.
 
  • #11
rcgldr said:
The small area of surface on the train that actually collides with the fly moves backwards, stops, and moves forwards again, same as the fly, for a very brief moment.
This is only the case in the frame of reference of the moving train, certainly not in the frame of reference of a stationary observer watching the collision from the side of the track.
 
  • #12
Chestermiller said:
This is only the case in the frame of reference of the moving train, certainly not in the frame of reference of a stationary observer watching the collision from the side of the track.
Which I clarified in post #8, but I've now added an update to post #3.

One issue is what is meant when an object touches another object. If some part of the fly's body is considered to be in contact with some part of the train during the collision, then there's some moment in time where the point of contact is stopped with respect to the ground. If the situation is viewed from the molecular level, then there is no contact, just a repulsive force due to the electrons and their related fields, and the force from the field changes the direction of the fly's body, without actual contact, only slowing down the trains molecules without stopping them, although I'm not sure what happens to the average position of the affected electrons.

Then again even in a solid, the molecules are bouncing around and I'm wondering if the maximum speed of molecules between collisions exceeds the forward speed of the train, in which case, part of the train is moving backwards for brief moments even without external collisions.
 
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  • #13
themagician said:
According to Newton laws the forces are equal,
That part's true.

themagician said:
and so, by this theory, the fly should stop the train.
How does that follow?
 
  • #14
rcgldr said:
Which I clarified in post #8, but I've now added an update to post #3.

One issue is what is meant when an object touches another object. If some part of the fly's body is considered to be in contact with some part of the train during the collision, then there's some moment in time where the point of contact is stopped with respect to the ground. If the situation is viewed from the molecular level, then there is no contact, just a repulsive force due to the electrons and their related fields, and the force from the field changes the direction of the fly's body, without actual contact, only slowing down the trains molecules without stopping them, although I'm not sure what happens to the average position of the affected electrons.

Then again even in a solid, the molecules are bouncing around and I'm wondering if the maximum speed of molecules between collisions exceeds the forward speed of the train, in which case, part of the train is moving backwards for brief moments even without external collisions.
The original question was almost certainly posed assuming that one could neglect what the individual molecules are doing. Within this framework, if the train is considered a rigid body, there is no way the leading edge of the train can ever have zero velocity during the collision.

Certainly the train is more rigid than the fly. So what happens to the fly? Well the fly is deformable, so when its leading edge encounters the leading edge of the train, the velocity at the leading edge of the fly changes instantaneously from its original velocity to the train velocity (assuming that the train has very large mass compared to the fly). But how can this be? The fly would have to have infinite acceleration. Well, no. The explanation is that the amount of mass involved in instantaneously changing the velocity of just the very leading edge of the fly is nil. The remainder of the fly is still traveling at the same velocity it had before its leading edge met the train. What happens is that a compression zone develops starting at the leading edge of the fly and propagating into the fly. This compression zone increases in length at essentially the speed of sound in the fly. The velocity of the part of the fly within the compression zone is equal to that of the train. The velocity of the part of the fly beyond the compression zone is equal to the original velocity of the fly. After the compression zone reaches the trailing edge of the fly, all parts of the fly are traveling with train velocity. During the collision, the force that the train exerts on the fly is equal to the linear density of the fly (assuming that the linear density is uniform) times the speed of sound in the fly times the velocity of the train.

Chet
 
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  • #15
Chestermiller said:
Certainly the train is more rigid than the fly. So what happens to the fly? Well the fly is deformable, so when its leading edge encounters the leading edge of the train, the velocity at the leading edge of the fly changes instantaneously from its original velocity to the train velocity (assuming that the train has very large mass compared to the fly).
Seems that the instant change in velocity would require a rigid train, not one that is just much more rigid than the fly. If the train isn't (infinitely) rigid, then any force exerted on the train results in some deformation at the point of contact. If the difference in velocity is great enough, then a less rigid object can end up penetrating the surface of the more rigid object (leaving a small dent), partly because the less rigid object becomes more dense and rigid due to compression.

Mythbusters had an episode where a piece of straw fired from an air gun at 320 mph penetrated about 1/4 inch into a palm tree. The myth was that the straw could go through the tree, which was busted, but the straw did end up embedded into the tree. Note the record for a high speed train is 374 mph.

http://mythbustersresults.com/episode61

http://kwc.org/mythbusters/2006/09/episode_61_deadly_straw_primar.html
 
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  • #16
rcgldr said:
Seems that the instant change in velocity would require a rigid train, not one that is just much more rigid than the fly. If the train isn't (infinitely) rigid, then any force exerted on the train results in some deformation at the point of contact. If the difference in velocity is great enough, then a less rigid object can end up penetrating the surface of the more rigid object (leaving a small dent), partly because the less rigid object becomes more dense and rigid due to compression.
Actually I was just trying to keep the discussion simple. A rigid train is definitely not required for the same basic principles to apply. In this case, however, the train will also experience a compressive wave that travels backwards from the contact patch, and both the train and the fly will experience an instantaneous change in velocity at the contact patch. The initial velocity at the patch will lie somewhere between that of the train and that of the fly but, of course, much much much closer to the train velocity.

Chet
 
  • #17
Chestermiller said:
The initial velocity at the patch will lie somewhere between that of the train and that of the fly but, of course, much much much closer to the train velocity.
That disparity would presumably fall out from the ratio of mass density times speed of sound in the fly (low) to mass density times speed of sound in the train (high)?
 
  • #18
jbriggs444 said:
That disparity would presumably fall out from the ratio of mass density times speed of sound in the fly (low) to mass density times speed of sound in the train (high)?
Yes, that would be part of it. But, in this problem, because of the complexity in geometry (fly shape, contact region that is small compared to train volume available for compressive wave to travel), the problem could not be modeled analytically.

Chet
 
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  • #19
I don't get the part about instantaneous change in velocity. Since even the smallest particle, perhaps just one electron, of the fly has some finite mass, then a finite change in vleocity will require a finite amount of time, since the collision force is not infinite. At some point that particle's velocity wrt ground is zero as it changes direction.

The real world effect is that the impact of the fly would cause some tiny abount of deformation on the trains surface during the early phase of the collision. Assuming the deformation is in the elastic range, the surface would recover back to it's original state.
 
  • #20
rcgldr said:
I don't get the part about instantaneous change in velocity. Since even the smallest particle, perhaps just one electron, of the fly has some finite mass, then a finite change in vleocity will require a finite amount of time, since the collision force is not infinite. At some point that particle's velocity wrt ground is zero as it changes direction.
If one models the fly and the train as continuous materials that interact through contact forces and which cannot interpenetrate then the conclusion follows.

The real world effect is that the impact of the fly would cause some tiny abount of deformation on the trains surface during the early phase of the collision. Assuming the deformation is in the elastic range, the surface would recover back to it's original state.
In the idealized model (with compressible materials) a deformation will occur. That does not mean that the velocity change of an infinitesimal portion of the contacting surfaces is not instantaneous. I believe that this is what Chester has in mind.
 
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  • #21
jbriggs444 said:
In the idealized model (with compressible materials) a deformation will occur. That does not mean that the velocity change of an infinitesimal portion of the contacting surfaces is not instantaneous. I believe that this is what Chester has in mind.
OK, but what could be considered the contact area has a finite size, it's not infinitesimal, so how to describe what happens to the contact area (where the two objects surfaces "touch"), using a contact model as opposed to:

http://sciencequestionswithsurprisinganswers.org/2013/04/16/do-atoms-ever-actually-touch-each-other
 
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  • #22
rcgldr said:
OK, but what could be considered the contact area has a finite size, it's not infinitesimal, so how to describe what happens to the contact area (where the two objects surfaces "touch"), using a contact model as opposed to:

http://sciencequestionswithsurprisinganswers.org/2013/04/16/do-atoms-ever-actually-touch-each-other
Again, the OPs question was asked and answered within the context of a continuum approach. If you wish to start a new thread on "what does it mean at the molecular level for bodies to make contact?", please feel free to do so. Continuing along these lines within the present thread is way beyond what the OP was asking, and may possibly confuse him/her.

Chet
 
  • #23
Chestermiller said:
Again, the OPs question was asked and answered within the context of a continuum approach. If you wish to start a new thread on "what does it mean at the molecular level for bodies to make contact?"
OK, but this gets back to my main question of how a contact area of finite (versus infinitesimal) size (therefore finite mass) could have instantaneous velocity change with a continuum approach. Example article (I've seen similar statements on youtube, doesnt' mean they are correct, but I did find a few of these):

When the train hits the fly, the fly does indeed stop the part of the train which it hits.

http://randomlyresearched.com/what-happens-when-a-fly-hits-a-train
 
  • #24
rcgldr said:
OK, but this gets back to my main question of how a contact area of finite (versus infinitesimal) size (therefore finite mass) could have instantaneous velocity change with a continuum approach.
Infinitesimal depth.
 
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  • #25
jbriggs444 said:
Infinitesimal depth.
Yes. A surface is 2D, and has no mass.

This thread is going nowhere, and I'm hereby closing it.

Chet
 

What is the "Train vs Fly" puzzle?

The "Train vs Fly" puzzle is a popular physics A level problem that asks which mode of transportation is faster for a long distance trip: a train or a fly. It involves considering the speed, distance, and time for each mode of transportation to determine the answer.

How do you solve the "Train vs Fly" puzzle?

To solve the "Train vs Fly" puzzle, you need to use the equation d = st, where d is the distance, s is the speed, and t is the time. You also need to consider the relative speeds of the train and fly, as well as any additional factors such as stops, delays, and wind speed.

What are the key principles of physics used in the "Train vs Fly" puzzle?

The "Train vs Fly" puzzle involves applying principles of relative motion, specifically the concept of frame of reference, which means considering the motion of objects from different points of view. It also involves using the formula d = st, which is a fundamental equation in physics that relates distance, speed, and time.

What are some common misconceptions about the "Train vs Fly" puzzle?

One common misconception about the "Train vs Fly" puzzle is that the answer is always the same, regardless of the specific parameters given. In reality, the answer can change based on the specific speeds, distances, and other factors involved. Another misconception is that the fly always wins, when in fact the train can also be faster depending on the circumstances.

How can the "Train vs Fly" puzzle be applied to real-life situations?

The "Train vs Fly" puzzle can be applied to real-life situations, such as deciding which mode of transportation to take for a long distance trip. It can also be used to understand the concept of relative motion in everyday scenarios, such as passing a car while driving or determining the best route for a race between two runners.

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