Crosswind problem (pgs. 34-35, Thinking Physics, 3rd edition)

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The discussion centers on understanding the concept of "artificial wind" in sailing, particularly in relation to the book "Thinking Physics" by Lewis Carroll Epstein. Participants clarify that when sailing directly downwind, the force on the sail decreases as the boat's speed matches the wind speed, causing the sail to sag. In contrast, when sailing across the wind, the relative airflow increases with boat speed, allowing for greater propulsion. The conversation highlights that a sail acts more efficiently like a wing when sailing across the wind rather than as a blunt body when going downwind. Ultimately, the mechanics of sailing across the wind can lead to higher speeds than sailing directly downwind, depending on various factors.
  • #241
Adress my
Gleb1964 said:
Here is your jet, as you wish. One in the ground frame and another in the cart frame. I have to split it in the volumes to illustrate somehow the transformation.

View attachment 322996
The jet CANNOT push the cart in the direction of the jet FASTER than the jet is going in the direction of the jet! No matter what you do to the sail orientation, or what angle you chose to go at relative to the incoming jet. Making anything you want variable... Momentum CANNOT enter ( nor exit) the cart at ##v_x = w##. The mass flow rate ##\dot m ## is a true "mathematical factor" in the sense that it is multiplied by anything you can come up with for the velocities- any configuration your heart desires. Short of DeVine intervention by the hand of GOD no matter what you do to the sail to maximize the acceleration of the cart there is a hard limit.

$$ \lim_{v_x \to v_j} \dot m = 0 \implies F_{nc} \to 0 $$

Period!
 
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  • #242
erobz said:
The jet CANNOT push the cart in the direction of the jet FASTER than the jet is going in the direction of the jet!
It certainly can. Just like the stick in the video below can push the cart in the direction of the stick faster than the stick is going in the direction of the stick.

 
  • #243
Bye.
 
  • #244
Here is the illustration, how slow wind (or jet) does collide with faster boat.

how slow wind collides with fast boat.png
 
  • #245
erobz said:
Stop with the apparent jet! Was there an "apparent jet" in the analysis?

Apparent just means relative to the cart. In your analysis that is the vector

$$\begin{pmatrix} v_j - v_c \\ 0 \end{pmatrix}$$
But for the boat going diagonally it has a y-component too.

1677509572796-png.png
 
  • #246
Gleb1964 said:
Here is your jet, as you wish. One in the ground frame and another in the cart frame. I have to split it in the volumes to illustrate somehow the transformation.

5-png.png
I don't think the orientation of the jet changes between the frames, just the velocity of the air particles, that the jet consists of.

5_AT.png


The jet is animated here in different frames:

 
  • #247
erobz said:
What you are proposing is not parallel to the agreed upon analysis technique shown in the video?
In your video the cart moves parallel to the jet, so even in the cart frame the incoming air in the jet still moves parallel to the jet.

But this is not the case if the cart moves diagonally, because here in the cart frame the air velocity is different from the jet orientation.

5_at-png.png


When you are trying to generalize from a simpler 1D-transformation (your video) to a more complex 2D-transformation, you have to be more careful.
 
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  • #248
A.T. said:
It certainly can. Just like the stick in the video below can push the cart in the direction of the stick faster than the stick is going in the direction of the stick.


That velocity vector is neither constant in magnitude nor direction over the duration of the push. It wobbles all over the place. There is a clear difference in direction in which the push begins and which the push ends. The labeled velocity vector at the end that was supposed to describe it perfectly over the duration of motion is a gross distortion of reality...as evidenced by the need for "velocity made good". Furthermore, if you pause the video an take some screenshots you'll see that cart has deviated from the assumed trajectory over the push as well. That is not a controlled experiment in the least bit. It's simply shoddy analysis, that leads to an absurd conclusion that goes against everything we learn in physics. It's a con artist tool.

This is no different conceptually than the little Pytagorean Puzzle, where it gets cut up and a square is suddenly missing. You are allowing yourself to be fooled.

This is precisely why vectors both magnitude and directions are so important. So when we get a result, we see that gross simplifications lead to deviation from perfect. We never say, lets adjust perfect!
 
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  • #249


erobz said:
That velocity vector is neither constant in magnitude nor direction over the duration of the push. It wobbles all over the place.
Do you seriously think it would stop working if the push was "cleaner". It is a kinematically constrained system, which can only move the way it does.

erobz said:
It's simply shoddy analysis, that leads to an absurd conclusion that goes against everything we learn in physics.
Which law of physics specifically do you see violated by this simple toy?
 
  • #250
A.T. said:
Do you seriously think it would stop working if the push was "cleaner". It is a kinematically constrained system, which can only move the way it does.Which law of physics specifically do you see violated by this simple toy?

None of the vectors that supposedly describe it are the reality! Everything is changing! The cart is on a curved trajectory! The pusher has neither controlled velocity nor constant direction. Everything is somewhat wrong.

You are being fooled!

https://en.wikipedia.org/wiki/Missing_square_puzzle#/media/File:Missing_Square_Animation.gif

This puzzle is proof positive of the very issue.

"velocity made good" is absolute madness.
 
  • #251


erobz said:
Everything is changing! from what it is upposed to be over the duration of the push.
It is a kinematically constrained system. The relative displacements will be the same, regardless if the speed is constant or not.
 
  • #252
A.T. said:
It is a kinematically constrained system. The relative displacements will be the same, regardless if the speed is constant or not.

All the directions are changing too.
 
  • #253
erobz said:
All the directions are changing too.
It would work even better, if it would wobble less. So what is your point?
 
  • #254
A.T. said:
It would work even better, if it would wobble less. So what is your point?
Bull. Its a simple perfect geomety problem. That "demonstration" is utter nonsense.
 
  • #255
erobz said:
bull.
Can we be grown ups now?
 
  • #256
A.T. said:
Can we be grown ups now?
That "demonstration" is utter nonsense. I am going to be a grown up and let you with you delusions.
 
  • #257

erobz said:
Its a simple perfect geomety problem.
Absolutely correct. The relative displacements are fully determined by simple geometry.

erobz said:
That "demonstration" is utter nonsense.
How does it contradict geometry?
 
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  • #258
A.T. said:
I don't think the orientation of the jet changes between the frames, just the velocity of the air particles, that the jet consists of.

View attachment 5_AT.png.webp
Ok, thank you for correction. You are right. I would need to think about it before posting.
 
  • #259
A.T. said:
How does it contradict geometry?
1677612541005.png


Its a rigid body on a track. Every point in the upper position is fully constrained and mapped by the right angle triangle to its lower position. If you end up with something else, things were bouncing sliding, bending, etc... Nothing was as it appeared to be, they are telling you a subtle lie, you are gobbling it up...asking for more...and worst of all...sharing it with others as "Physics"!
 
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  • #260
erobz said:
1677612541005-png.png


Its a rigid body on a track. Every point in the upper position is fully constrained and mapped by the right angle triangle to its lower position.

Good start. Now add the pushing stick for both positions.

I would also recommend rotating the vane slightly clockwise, so its orientation bisects the angle between vertical and track. This will make the illustration clearer.
 
  • #261
A.T. said:
Good start. Now add the pushing stick for both positions.

I would also recommend rotating the vane slightly clockwise, so its orientation bisects the angle between vertical and track. This will make the illustration clearer.
That red arrow is the change in length of the pushing stick. Bye. This time its for real.
 
  • #262
erobz said:
That red arrow is the change in length of the pushing stick.
Wrong. Draw the stick in both positions. It must touch the vane for both positions, and be only displaced horizontally.
 
  • #263
A.T. said:
Wrong. Draw the stick in both positions. It must touch the vane for both positions, and be only displaced horizontally.
Ahh. S.o.b. There is some kind of mechanical advantage here. Are you breaking me like a wild stallion...maybe a pony?

1677616700561.png
 
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  • #264
erobz said:
There is some kind of mechanical advantage here.
Absolutely, and so is in sailing.
 
  • #265
A.T. said:
Absolutely, and so is in sailing.
So then the analysis I was trying to get to before this will reveal this mech advantage too...if I do it properly?
 
  • #266
erobz said:
So then the analysis I was trying to get to before this will reveal this mech advantage too...if I do it properly?
If I understand your aim correctly, it was about checking momentum conservation. Mechanical advantage roughly means that you can trade force for speed without violating energy conservation.
 
  • #267
A.T. said:
If I understand your aim correctly, it was about checking momentum conservation. Mechanical advantage roughly means that you can trade force for speed without violating energy conservation.
Don't worry, you won't have to worry about correcting me anymore today. I'm already going to be in trouble for this one.

Thanks for your help, I let my emotions get the best of me. I'm sorry.
 
  • #268
erobz said:
Thanks for your help, I let my emotions get the best of me. I'm sorry.
No problem. Here is another mechanical analogy: A thin wedge squeezed between oblique surfaces:

 
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  • #269
1677768557166.png


The frame is fixed to the origin (not the control surface), ##\boldsymbol{i}## parallel to the slope.

I'm trying to find the velocity of the jet "##v_j## relative to the cart:

$$ v_{j/O} \boldsymbol{i} = v_{j/c} \boldsymbol{i} + v_{c/O} \boldsymbol{i} \implies v_{j/c} \boldsymbol{i} = \left( v_j \cos \theta - v_c \right) \boldsymbol{i} $$

$$ v_{j/c} \boldsymbol{j} = -v_j \sin \theta \boldsymbol{j}$$

That means the magnitude of ## \vec{v}_{j/c}## is given by:

$$ \left| v_{j/c} \right| = \sqrt{ \left( v_j^2 - 2 v_j v_c \cos \theta + v_c^2 \right) }$$

Letting ##\cos \theta \to 0 ## looks as expected:

$$\lim_{\theta \to 0 } \left| v_{j/c}\right| = \sqrt{v_j^2 - 2 v_j v_c + v_c^2} = \sqrt{\left( v_j - v_c\right)^2} = v_j- v_c$$

However, the limit as ##\theta \to 90°##:

$$\lim_{\theta \to 90° } \left| v_{j/c}\right| = \sqrt{v_j^2 + v_c^2} $$

That seems unlikely. What have I goofed on already?
 
  • #270
erobz said:
I'm trying to find the velocity of the jet "##v_j## relative to the cart:
There are two relative velocities of jet, relative to cart and relative to the sail. Jet is crossing the planar sail, the velocity regarding to this crossing point is not the same, as velocity regarding to the cart.
8.png
 
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