Why Do Objects Only Reach 95% of Their Terminal Velocity?

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Discussion Overview

The discussion revolves around the concept of terminal velocity and why falling objects are said to reach approximately 95% of their theoretical terminal velocity rather than achieving it completely. Participants explore the implications of drag force, the mathematical modeling of motion, and the effects of atmospheric conditions on terminal velocity.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that terminal velocity is never fully reached due to the nature of drag force, which is proportional to velocity, leading to an asymptotic approach to terminal velocity.
  • Others argue that while terminal velocity is theoretically approached, practical considerations allow for a figure like 95% to be deemed "close enough" for real-world applications.
  • A participant explains that the differential equation governing motion shows that as velocity increases, the net force decreases, making it increasingly difficult to reach terminal velocity.
  • Some contributions highlight that changes in atmospheric density with altitude can affect the drag force and thus the terminal velocity experienced by an object falling from high altitudes.
  • A related analogy is presented comparing the scenario to walking half the remaining distance to a wall, suggesting that while one may never mathematically reach the wall, a practical limit is recognized.
  • Another participant notes that the exponential nature of the equation indicates that terminal velocity is approached asymptotically, reinforcing the idea that it is never fully attained.

Areas of Agreement / Disagreement

Participants generally agree that terminal velocity is approached asymptotically and that practical applications often accept 95% as sufficient. However, there is no consensus on the implications of this for real-world scenarios, particularly regarding the effects of changing atmospheric conditions and the mathematical modeling of motion.

Contextual Notes

Limitations include assumptions about constant gravity and drag proportionality, as well as the complexity introduced by varying atmospheric density at different altitudes, which may affect the terminal velocity experienced by falling objects.

bbq2014
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Hi forum!

Why can't falling objects reach terminal velocity in the real world?

When an object drops (W = mg) it will experience drag force upwards. And since drag is proportional to velocity, both force will eventually be equal therefore, the object will not accelerate anymore, hence reaching terminal velocity.

So why is it assumed that the object is at terminal velocity when the object has reached 95% of its theoretical terminal velocity?

Are they assuming this in an ideal world where there is no air resistance and since in object will reach terminal velocity when t = ∞, and since an exponential function will never reach 0, terminal velocity cannot be reached?

Thank you for reading this!
 
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bbq2014 said:
So why is it that we say ...
Who is "we"? Reference? Context?

If the terminal velocity is just an estimate with +/- 5% accuracy then it makes sense to say that.
 
bbq2014 said:

Why can't falling objects reach terminal velocity in the real world?

When an object drops (W = mg) it will experience drag force upwards. And since drag is proportional to velocity, both force will eventually be equal therefore, the object will not accelerate anymore, hence reaching terminal velocity.


If you assume a model where drag is proportional to velocity, gravity is constant and the atmosphere does not get thicker as you descend then the difference between actual velocity and terminal velocity will decay exponentially. The two will never be exactly equal.

If you change the drag formula, the decay may no longer be exponential. But (barring fairly exotic drag formulae) the result will still be that actual velocity approaches terminal velocity asymptotically. You'll hit the ground before they can become equal. Still, you can get close enough for practical purposes. 95% is a reasonable figure for "close enough".

[If you allow for changes in atmospheric density with altitude, it is possible to have a falling object (momentarily) hit terminal velocity exactly. But that's often a more complex model than the situation warrants -- it's easier to pretend that "terminal velocity" is a constant]
 
jbriggs444 said:
If you assume a model where drag is proportional to velocity, gravity is constant and the atmosphere does not get thicker as you descend then the difference between actual velocity and terminal velocity will decay exponentially. The two will never be exactly equal.

Hi jbriggs Could you elaborate more into why it can never be equal? What if you could scale this scenario up, let say you dropped it from the edge of the atmosphere? Is it due to the changing air density at different altitudes which changes the drag? Thank you!
 
bbq2014 said:
Hi jbriggs Could you elaborate more into why it can never be equal?
The differential equation of motion would be v'(x) = g - kv(x). If you are able to solve differential equations, this is an easy one and the solution involves an exponential.

Looking at it from a more simplistic viewpoint, suppose that you jump out of a hot air balloon. You are falling at 0 mph. Your terminal velocity is (let's say) 100 mph.

You fall for one second against negligible wind resistance, gaining roughly 20 mph. Now wind resistance is equal to about 20% of gravity.

You fall for another second against this wind resistance. This time you gain only 80% of 20 mph. That's another 16 mph for a total of 36 mph. Now wind resistance is equal to 36% of gravity.

You fall for another second against this wind resistance. This time you gain only 64% of 20 mph. That's another 12.8 mph for a total of 48.8 mph. Call it 50 mph. Now wind resistance is equal to 50% of gravity.

The closer your speed gets to terminal velocity the slower your speed increases. It never quite gets there. The difference decays geometrically. It took you three seconds to go from a 100 mph delta to a 50 mph delta. It will take another three seconds to get to a 25 mph delta. Another three to get to a 12.5 mph delta. Another three to get to a 6.25 mph delta.

So after 12 seconds, you're roughly at 95% of terminal velocity.

[The difference between the simplistic picture and the differential equation is that the differential equation is the ideal limit as one does the simplistic calculation using smaller and smaller time intervals]

What if you could scale this scenario up, let say you dropped it from the edge of the atmosphere? Is it due to the changing air density at different altitudes which changes the drag?
If you factor in the changes in air density, then "terminal velocity" starts out quite high at the edge of the atmosphere and reduces to more normal values as one descends. So a falling astronaut will fall at a high rate of speed initially (greater than the speed of sound). As he falls into denser air the corresponding terminal velocity will be decreasing. He will eventually be going faster than the [reduced] terminal velocity and will be slowing down rather than speeding up.
 
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bbq2014 said:
Hi jbriggs Could you elaborate more into why it can never be equal?
The closer you get to terminal velocity, the smaller the net force that accelerates you.
 
Related problem...

Stand 20ft from a wall. Every 5 mins walk forwards half the remaining distance to the wall. How long will it take to reach the wall? In theory never. In practice at some point you will decide you are close enough.
 
Since the equation is exponential and terminal velocity is the asymptotic, it is easy to see mathematically that you never reach it. 95% is just a common, convenient "close enough".
 

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