Fluids and Ping Pong Ball Magnus and Coanda Effect

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Discussion Overview

The discussion revolves around the behavior of a ping pong ball suspended in a jet of air from a hairdryer, exploring the roles of the Magnus effect and the Coanda effect in this phenomenon. Participants examine the stability of the ball, the effects of airflow, and the principles of fluid dynamics involved, including concepts of pressure gradients and flow separation.

Discussion Character

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

Main Points Raised

  • Some participants propose that the stability of the ping pong ball in the air jet is due to a decrease in pressure caused by the high velocity of the jet, which keeps the ball from flying off.
  • Others argue that the Magnus effect may play a role if the ball is spinning, suggesting that the jet's angle could cause the ball to spin and affect its trajectory.
  • It is noted that the Magnus effect requires rotation, and without it, the effect does not apply, leading to questions about the relevance of the ball's rotation in this context.
  • Some participants clarify that the Coanda effect describes how a fluid adheres to a surface, but there are conditions under which flow can separate from an object, raising questions about predicting flow attachment versus separation.
  • There is a discussion about how turbulent wakes behave differently from laminar wakes, with some suggesting that turbulent flow can resist separation better due to higher momentum near the surface.
  • Participants express skepticism about the term "Coanda effect," suggesting it is often misused and that the behavior of fluids can be explained by standard fluid dynamics principles without invoking special rules.
  • Questions arise regarding the relationship between pressure gradients and flow behavior, particularly in the context of how pressure changes affect flow attachment and separation.
  • One participant seeks clarification on a specific example involving a jet and a plate, questioning the explanation provided in external sources about pressure differences affecting the jet's behavior near the plate.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the roles of the Magnus effect and Coanda effect, with multiple competing views and ongoing questions about fluid dynamics principles. The discussion remains unresolved regarding the specific contributions of these effects to the behavior of the ping pong ball.

Contextual Notes

Limitations include the complexity of fluid dynamics concepts such as pressure gradients, flow attachment, and separation, which are not fully resolved in the discussion. The relationship between the Coanda effect and general fluid behavior is also debated without definitive conclusions.

member 428835
Hi PF!

Given a hairdryer blowing vertically against gravity toward a ping pong ball the ping pong ball is suspended. The ball is relatively stable in the jet because the high velocity of the jet causes a decrease in pressure, causing the ambient air to mix, therefore keeping the ball in the jet rather than flying off sporadically.

If the hair dryer is angled to the right, the ping pong ball still floats. Is this solely due to the above explanation or does the Magnus effect play a role? I was thinking that with the jet toward the right, the ball would spin clockwise, thereby forcing the wake of the ball to the bottom right. The equal and opposite force of the air would then push the ball to the upper left.

As far as I understand, the Coanda effect forces the air to adhere to the curvature of the ball, but can someone explain why this happens and how this force of adhering to the wall differs from the Magnus effect (which seems to explain why the wake redirects)?

Thanks!
 
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Well, for one, the Magnus effect requires the ball to be rotating, and generally fairly rapidly. No rotation, no Magnus effect. The Coanda effect is solely due to the fact that a fluid can't form a void, so a jet near a surface will stick to it.
 
boneh3ad said:
Well, for one, the Magnus effect requires the ball to be rotating, and generally fairly rapidly. No rotation, no Magnus effect.
But the ping pong balls do rotate when above an air dryer; do you think this is relevant to suspending the ball?

boneh3ad said:
The Coanda effect is solely due to the fact that a fluid can't form a void, so a jet near a surface will stick to it.
But sometimes flow separates from objects and leaves recirculating flow, not flow that remains attached. How then can we predict when the flow remains attached rather then separates?

Perhaps related, but I know turbulent wakes along a sphere separate later along the sphere's surface than laminar wakes, presumably because the higher momentum near the surface for the turbulent case can resist the wake's adverse pressure gradient further than in the laminar case. Is the Coanda effect related?
 
joshmccraney said:
But the ping pong balls do rotate when above an air dryer; do you think this is relevant to suspending the ball?

No, that is generally just due to differential shear on the sides of the ball since jets like a hair dryer are highly turbulent and unsteady.

joshmccraney said:
But sometimes flow separates from objects and leaves recirculating flow, not flow that remains attached. How then can we predict when the flow remains attached rather then separates?

That flow is still attached in the sense that there is no void touching the surface. There is still air there. That's a different phenomenon known as separation. After all, the Coanda effect isn't all-powerful. Eventually, other factors will be great enough to force the jet to separate from the surface, at which point other fluid is drawn under it so that still no void forms.

When does separation occur? Basically, when a boundary layer experiences an adverse pressure gradient for long enough, it will develop a region of reversed flow near the surface. This is separation.

joshmccraney said:
Perhaps related, but I know turbulent wakes along a sphere separate later along the sphere's surface than laminar wakes, presumably because the higher momentum near the surface for the turbulent case can resist the wake's adverse pressure gradient further than in the laminar case. Is the Coanda effect related?

That's correct. The Coanda effect is related in the sense that a boundary layer forms and undergoes the same exact rules as any other boundary layer. This is why I really hate when people throw around the term "Coanda effect" as if it is some kind of special rule, when really it's just fluids behaving normally. In fact, in all of the fluids courses I have taken or taught, I have never once "learned" or "taught" the Coanda effect. It's just normal fluid motion.
 
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boneh3ad said:
No, that is generally just due to differential shear on the sides of the ball since jets like a hair dryer are highly turbulent and unsteady.
Thanks for the clarification!

boneh3ad said:
That flow is still attached in the sense that there is no void touching the surface. There is still air there. That's a different phenomenon known as separation. After all, the Coanda effect isn't all-powerful. Eventually, other factors will be great enough to force the jet to separate from the surface, at which point other fluid is drawn under it so that still no void forms.
So am I correct in saying that the Coanda effect occurs everywhere along the ball until separation?

boneh3ad said:
That's correct. The Coanda effect is related in the sense that a boundary layer forms and undergoes the same exact rules as any other boundary layer. This is why I really hate when people throw around the term "Coanda effect" as if it is some kind of special rule, when really it's just fluids behaving normally. In fact, in all of the fluids courses I have taken or taught, I have never once "learned" or "taught" the Coanda effect. It's just normal fluid motion.
Interesting; I've only just learned of it but this is good to know! So you're saying fluids flow around an object 1/2 ways: either the flow remains attached, perhaps due to momentum and inertia overpowering the adverse pressure gradient, or the flow separates, signifying the momentum has decreased to the point where the pressure gradient dominates. Both of these situation arise from fluid "not forming a void", although the former is sometimes referred to as the Coanda effect? Have I said this correct?

Lastly, I saw on a wikipedia page regarding the Coanda effect a picture of a jet with a plate near the bottom side. In a picture a moment later the jet tends toward the plate. Their explanation is that the pressure underside the jet is lower than that above the jet, causing fluid to tend toward the plate. My intuition says since the plate is not moving, no slip implies velocities tend to be lower underside, and hence pressure should be higher, which I feel would push the jet away from the wall. Can you explain this?
 
I wouldn't say the pressure gradient dominates. Consider the flow over the top of an airfoil, for example. For about the first half, the flow accelerates over the upper surface under the influence of a favorable pressure gradient. That velocity profile is going to look a little "fuller" at the top than what you would expect from a simple Blasius profile. After it passes that top point, called the pressure minimum, it now encounters a region of increasing pressure. Over the rest of the wing, the adverse pressure gradient slowly removes momentum from the boundary layer. If that adverse pressure gradient persists for long enough, it can cause the flow near the wall to reverse, forming a separation bubble.

So it's not a matter of the pressure gradient necessarily dominating. It's really just a matter of the pressure gradient acting over a distance that is large enough that some region of the fluid decelerates back down to zero velocity and then continues on to a negative velocity.
 
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Gotcha! Thanks a ton! did edit my post 5; would you mind reading the last part regarding the jet and wall (which I call a plate, though it shouldn't matter)?
 

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