Why does air resistance increase with speed?

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Discussion Overview

The discussion centers on the relationship between air resistance and speed, exploring the underlying mechanisms from a particle theory perspective. Participants examine how air resistance, or drag force, varies with velocity and surface area, and the implications of these factors in different contexts, including theoretical and practical applications.

Discussion Character

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

Main Points Raised

  • Some participants propose that air resistance increases with speed due to more air molecules colliding with the object as it moves through the air.
  • Others argue that the number of air molecules hitting the body is proportional to the surface area, which remains constant, leading to confusion about the relationship with speed.
  • A participant explains that a moving object must push air out of the way, transferring kinetic energy to the air, which increases with speed.
  • Some contributions highlight that drag force can be proportional to the square of the velocity, particularly at higher speeds, while others note that at lower speeds, drag can be linear.
  • There is mention of Stokes' law, which describes drag for a sphere in a viscous fluid, indicating that drag can vary based on the fluid's properties and the object's speed.
  • Participants discuss the role of turbulence and how energy imparted to air molecules at the front of an object may not be fully recovered at the back, contributing to drag.
  • Some participants question the simplifications made in earlier posts, emphasizing the need to consider the mean speed of air molecules and the complexities of turbulence in understanding drag.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the relationship between air resistance, speed, and surface area. The discussion remains unresolved, with no consensus on the exact nature of these relationships or the best explanatory models.

Contextual Notes

Some participants note that the density of air changes with altitude, which could affect drag, and that the factor of proportionality between air resistance and area may vary with other variables, such as velocity. The discussion includes references to different drag models and conditions under which they apply.

Who May Find This Useful

This discussion may be of interest to high school physics students, educators, and anyone exploring the principles of fluid dynamics and the factors affecting drag forces in various contexts.

ap_cycles
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HI,

My question as per above.

A quick check with Physicsclassroom.com reveals that a (perhaps too simplistic) reason is that more and more air molecules are hitting the body as the body falls through the air. But i am confused. I thought when the body first falls through the air fluid, the number of air molecules hitting the body is proportional to the surface area of contact, which as we all know, is fixed (body shapes don't change right!).

I understand that air resistance is a form of drag force, and this drag force is dependent on velocity of the falling body. What i want to know, however, is how we can explain this phenomena in terms of particle theory.

Fellow forummers help me please? A high school physics teacher here. :wink:
 
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Now, let us have a body with a front surface with area A moving with velocity V.

In a time interval dt, then, the region of space the surface has traversed has the volume A*V*dt.
Multiplying this with the molecular density yields the amount of molecules displaced during that time interval.

If you reduce the velocity, fewer molecules will be displaced in the same time interval, and thus, give rise to less air resistance.
 
If you have still air, as you could say you have at the beginning of the fall, the air molecules still have velocities associated with them when they hit you. Their average velocity is just 0, but they still have velocities individually! So sure, it makes sense that the only thing that matters if how much surface area you have, but that's only at rest. Now consider, to make the point clearer in my opinion, not a person falling through the atmosphere at 200mph, but a person standing still being pummeled by 200mph wind. Now, of course more surface area would still mean more wind bouncing off of your, but 200mph plus or minus each individual molecules velocity when the air is at rest as a whole is a far greater force then at rest.
 
A moving object has to push the air out of the way and transfer some kinetic energy to that air.You can feel this when you stand by the side of the road and a speeding car goes past.If the object moves faster it moves a greater mass of air per second and gives that air a greater increase of speed.Perhaps you could ask your students to make fans and then feel the effects of fanning themselves at different speeds.
 
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arildno said:
Now, let us have a body with a front surface with area A moving with velocity V.

In a time interval dt, then, the region of space the surface has traversed has the volume A*V*dt.
Multiplying this with the molecular density yields the amount of molecules displaced during that time interval.

If you reduce the velocity, fewer molecules will be displaced in the same time interval, and thus, give rise to less air resistance.

Yes, well, drag is, to first approximation, in proportion to the square of the velocity.
 
I thought when the body first falls through the air fluid, the number of air molecules hitting the body is proportional to the surface area of contact, which as we all know, is fixed (body shapes don't change right!).
don't forget that at the height the object was dropped, the density of air molecules is a lot less than that at ground level. air is " thin" at jump altitude. It is a lot ' thicker ' at ground level. Air also exerts about 14 psi pressure at at ground level. the object will fall at an increasing rate until it reaches terminal velocity.
 
To Phrak, Dadface, Pengwuino, arildno,

Thank you very much for all of your replies!

Now i understand... :!)
 
Phrak said:
Yes, well, drag is, to first approximation, in proportion to the square of the velocity.
That depends on what sort of drag you are talking about. It really is a very complicated phenomenon.

If you take Stoke's law of resistance for a sphere moving through a viscous fluid, that drag is linear in the velocity. (The drag due to viscous forces is a different mechanism than molecular displacement). Stokes' law is extremely accurate, and has many practical applications .

If you work with an inviscid fluid, where the fluid is locally stationary in respect to a non-accelerating body, then you'll end up in..D'Alembert's paradox.

It is cerainly true that for relatively high speeds, a square velocity law is generally best, but for low speeds, a linear model for air resistance is often accurate enough.


Thus, I chose not to delve into intricacies of modelling, but to point to one omni-present feature that points in the direction of the relation increased speed-increased air resistance.

I didn't tell the whole story, not the least because many features of that story is not known by me.
 
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What is happening at the front of the object is only a small part of the story. With laminar flow, the energy you impart to the molecules at the front, by shifting them out of the way, (force times distance, effectively) should be returned at the back end as they come together again (particularly true if you take an object tapered at both ends, to make it simple and with a fluid of low/no viscosity).
But, once you start gong fast, the energy used in pushing the air aside at the front, is lost in the form of turbulence and it's not 'available' to push back together at the back. This is detected as a drop in pressure at the back (drag).
It's often worth while using an intermediate step in reasoning about these things and not making yourself explain everything in terms of particles, the whole way through.
 
  • #10
ap_cycles said:
A quick check with Physicsclassroom.com reveals that a (perhaps too simplistic) reason is that more and more air molecules are hitting the body as the body falls through the air. But i am confused. I thought when the body first falls through the air fluid, the number of air molecules hitting the body is proportional to the surface area of contact, which as we all know, is fixed (body shapes don't change right!).
Why can't it be proportional to both? Or proportional to one and proportional to the square of the other...?
 
  • #11
In high school, russ, "proportional" means there exists a proportionality constant, rather than that the ratio between two proportional quantities should be independent of those quantities..
 
  • #13
russ_watters said:
I don't see your point.
The factor of proportionality between air resistance&area might (and does) vary with some third variable (but not with either of those two).
If OP thought the proportionality factor was a constant, and couldn't be a function of, say, velocity, then his question makes some sort of sense.

Just speculating..
 
  • #14
You are talking as if the molecules of air are all stationary. In fact, the mean speed of the air molecules is much higher than that of a falling object. Molecules will be hitting the back as well as the front of your object. Being so simplistic about the situation doesn't help at all with understanding what's going on.
You have to consider turbulence or you would have to say that all objects of the same cross sectional area would have the same drag factor. A number of Formula One designers might disagree with you there.
 
  • #15
arildno said:
The factor of proportionality between air resistance&area might (and does) vary with some third variable (but not with either of those two).
If OP thought the proportionality factor was a constant, and couldn't be a function of, say, velocity, then his question makes some sort of sense.

Just speculating..
If you hold area constant and vary the speed, then you have drag as proportional to velocity squared. If you hold velocity constant and vary the area, then you have drag proportional to the area.
 

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