Fuzzy
Member
I used to play golf. Badly. I played again recently and it got me thinking about dimples and turbulence.
Golf balls are dimpled. The dimples create tiny pockets of low pressure in flight that allow the ball to travel faster and, if well hit, straighter. (This also allows you to radically curve the ball too). Bernoulli's principle at work, essentially.
What would happen, then, if you were to apply the same technology to an arrow? The folowing is a thought experiment:
Imagine two arrows: arrow 1 has a point. The head of the point remains sharp; the rest is covered in tiny dimples. The shaft is similarly dimpled, with an undimpled area at the back for fletches etc. Arrow two is identical to arrow one apart from the dimpling.
When shot, these arrows spin, like all arrows. They both move forwards and rotate about their long axes. If you're a non-compounder, they moving significantly from side to side due to "paradox".
Ignoring the relatively massive drag effect of fletchings (which, if they are fletched the same, should cancel out), what, if any, is the difference between these two arrows?
Arrow 2 flies normally, but...
Arrow 1 is generating low-pressure spots as it moves forwards and rotates. I imagine that the point is where this effect would be most marked, although the same effect must apply along the length of the arrow too. I reckon this arrow will:
Move marginally faster through the air due to these low pressure areas.
Rotate faster, as the effect of those low pressure spots also apply in the direction of spin.
Might move slightly in the direction of lateral spin.
Might also suffer increased drag from side-to-side movement as the airflow is more disturbed (dimples again).
What do you think? Fluid dynamicists especially welcome - and if anyone has a physics modelling package and some spare time to play with, I'd be fascinated at the results.
Golf balls are dimpled. The dimples create tiny pockets of low pressure in flight that allow the ball to travel faster and, if well hit, straighter. (This also allows you to radically curve the ball too). Bernoulli's principle at work, essentially.
What would happen, then, if you were to apply the same technology to an arrow? The folowing is a thought experiment:
Imagine two arrows: arrow 1 has a point. The head of the point remains sharp; the rest is covered in tiny dimples. The shaft is similarly dimpled, with an undimpled area at the back for fletches etc. Arrow two is identical to arrow one apart from the dimpling.
When shot, these arrows spin, like all arrows. They both move forwards and rotate about their long axes. If you're a non-compounder, they moving significantly from side to side due to "paradox".
Ignoring the relatively massive drag effect of fletchings (which, if they are fletched the same, should cancel out), what, if any, is the difference between these two arrows?
Arrow 2 flies normally, but...
Arrow 1 is generating low-pressure spots as it moves forwards and rotates. I imagine that the point is where this effect would be most marked, although the same effect must apply along the length of the arrow too. I reckon this arrow will:
Move marginally faster through the air due to these low pressure areas.
Rotate faster, as the effect of those low pressure spots also apply in the direction of spin.
Might move slightly in the direction of lateral spin.
Might also suffer increased drag from side-to-side movement as the airflow is more disturbed (dimples again).
What do you think? Fluid dynamicists especially welcome - and if anyone has a physics modelling package and some spare time to play with, I'd be fascinated at the results.