What Causes Raindrops to Follow a Tail on a Train Window?

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Discussion Overview

The discussion revolves around the phenomenon of raindrops following a tail on a train window, exploring the underlying physical principles and mechanisms involved. Participants examine aspects of fluid mechanics, surface tension, and molecular interactions, while questioning the stability and behavior of the water trails formed on the glass surface.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant notes that raindrops appear to follow parabolic trajectories influenced by gravity and wind, and questions the stability of the water tail left behind.
  • Another participant attributes the tendency of raindrops to follow trails to the cohesive properties of water molecules, specifically the hydrogen bonds that attract them to each other.
  • A different viewpoint suggests that two processes are at play: the weak bonding of water molecules to the glass surface and the surface tension of water, which seeks to minimize potential energy and maximize the volume-to-surface ratio.
  • This participant also mentions that the water trail is mechanically metastable and can break apart due to disturbances, leading to the formation of round droplets.
  • One participant challenges the observations by referencing the 'no-slip boundary condition' in fluid mechanics, indicating that the complete understanding of the phenomenon remains an area of active research.
  • Contact line motion is highlighted as a significant aspect of the discussion, with references to ongoing research in the field.

Areas of Agreement / Disagreement

Participants express differing views on the mechanisms behind the observed phenomenon, with no consensus reached on the primary causes or the implications of the observations. The discussion remains unresolved regarding the fundamental principles at play.

Contextual Notes

Participants acknowledge the complexity of the phenomenon, including the interplay of surface tension, molecular attraction, and the implications of the no-slip boundary condition, which remains a debated topic in fluid mechanics.

ChrisVer
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Today I was taking the train to a nearby city, where we passed through some rainy region.
As the raindrops fell on the window, one could see their trajectories almost followed a parabola depending on their initial conditions. That is something expected, due to gravity and the forces acted on them by the running wind.
However as you see them moving, they leave behind a water tail - something like a stream-, and that tail is the preferred way the rest drops will follow (they move up to it, and then they follow it). Why is this happening?
Also if there are no more drops to follow that tail, it will suddenly break apart to stationary drops. Why is this happening? I don't think it's due to statistics, because if it was that, you wouldn't see the whole line to be divided simultaneously. It's more like, due to tension forces on the water, it's an unstable "structure"- under some perturbations it falls apart all together.
I hope I made the questions clear. Looking forward to your answers.
 
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I can say that the reason why rain drops will tend to follow the trails of other drops is because of the property known as cohesion. As water molecules come close to one another the hydrogen bonds attract the molecules together.
 
I think there are two processes going.

The first is attraction between glass and water molecules. Glass is slightly hydroscopic, so water molecules can bond very weakly to the glass surface. This will tend to flatten the water drop that is in contact with the surface. This is basic surface wetting.

The second is surface tension of water. The system of water molecules will try to arrange itself to minimize its potential energy, which means minimizing total surface tension, which basically translates to maximizing volume-to-surface ratio. So a droplet, in absence of other forces, will be perfectly spherical.

So hydroscopic attraction will try to spread the water out, and surface tension will try to gather it up. The result is the trail that you see. A water trail is probably only metastable mechanically, so some mechanical disturbance (like the car shaking, or air turbulence) will shift it into the other stable state - a round droplet. When this happens, the trail breaks up.

The attraction also acts as friction. Attraction obviously drops off with distance from the surface. So a trail can sort of "shield" new droplets from the surface. They experience less friction and can travel faster along a trail.
 
ChrisVer said:
<snip> Why is this happening?
<snip>

You have observed a simple phenomenon that contradicts a central assertion in fluid mechanics: the 'no-slip boundary condition'.

http://en.wikipedia.org/wiki/No-slip_condition

The complete answer to your question is still unknown- if you read the last few sentences in the 'exceptions' section above. Another good description of the no-slip condition is here:

http://arxiv.org/pdf/cond-mat/0501557.pdf

To your specific questions, you are observing contact line motion, which is still an active area of fundamental research:

http://www.annualreviews.org/doi/abs/10.1146/annurev-fluid-011212-140734
 

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