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Stone Skipping Tom as Cruz Lu s Cebola Stone Shape Angle With - - PowerPoint PPT Presentation

Stone Skipping Tom as Cruz Lu s Cebola Stone Shape Angle With Water Spin Childrens Game? Childrens Game? Physics of Everyday Life Physicists have figured out some extremely fine details of the universe, from the radius of


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SLIDE 1

Stone Skipping

Tom´ as Cruz Lu´ ıs Cebola

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SLIDE 2

Stone Shape

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SLIDE 3

Angle With Water

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SLIDE 4

Spin

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SLIDE 5

Children’s Game?

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SLIDE 6

Children’s Game?

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SLIDE 7

Physics of Everyday Life

“Physicists have figured out some extremely fine details of the universe, from the radius of black holes to the behavior of subatomic particles - neither of which we can even see. It may surprise you to learn, then, that they lack explanations (or have

  • nly recently stumbled upon them) for many common phenomena

we observe in daily life.” − Natalie Wolchover

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SLIDE 8

Physics of Everyday Life

“Physicists have figured out some extremely fine details of the universe, from the radius of black holes to the behavior of subatomic particles - neither of which we can even see. It may surprise you to learn, then, that they lack explanations (or have

  • nly recently stumbled upon them) for many common phenomena

we observe in daily life.” − Natalie Wolchover

The Cheerios Effect

Why your breakfast cereal tends to clump together or cling to the sides of a bowl of milk? - See Vella and Mahadevan, The ’Cheerios effect’.

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SLIDE 9

Getting a Kick From Water

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SLIDE 10

Getting a Kick From Water

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SLIDE 11

A Simple Model 1

Reaction Force

◮ Re = aV

ν ∼ 105 ⇒ Inertial regime.

◮ We = ρV 2z

σ

∼ 100 ⇒ Neglect surface tension.

◮ Fr = V 2

zg ≫ 1 ⇒ Neglect buoyancy.

F = 1 2ClρwV 2Simf (θ, β)n

  • Lift

+1 2CdρwV 2Simf (θ, β)t

  • Drag

1Based on: Rosellini et al, 2005 e Boqcuet L, 2002.

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SLIDE 12

A Simple Model 1

Reaction Force

◮ Re = aV

ν ∼ 105 ⇒ Inertial regime.

◮ We = ρV 2z

σ

∼ 100 ⇒ Neglect surface tension.

◮ Fr = V 2

zg ≫ 1 ⇒ Neglect buoyancy.

F = 1 2ClρwV 2Simf (θ, β)n

  • Lift

+1 2CdρwV 2Simf (θ, β)t

  • Drag

Stone Shape: Immersed Surface

Sim = R2

  • arccos
  • 1 − s

R

  • 1 − s

R 1 −

  • 1 − s

R 2

  • , s = |z|

sin θ

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SLIDE 13

A Simple Model

Spin?:

What is the effect of spinning?

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SLIDE 14

A Simple Model

Spin?:

What is the effect of spinning?

  • 1. Lift force is applied in the

immersed surface - destabilizing torque;

  • 2. Only a specific range of θ is

favourable to skipping;

  • 3. Gyroscopic effect - Stabilizing

torque;

¨ θ + In − It It ˙ φ 2 (θ − θ0) = Mθ It (θ − θ0) ∼ MθIt ˙ φ2(In − It)2 To work ˙ φ 20Hz.

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SLIDE 15

A Simple Model

To address the problem of the angle we need to go deeper in the model

x = − 1

2ρ(˙

x2 + ˙ z2)Sim(z) sin(θ + β)(Cl sin θ + Cd cos θ) M¨ z = −Mg + 1

2ρ(˙

x2 + ˙ z2)Sim(z) sin(θ + β)(Cl cos θ − Cd sin θ) Notice that: β = arctan −˙

z ˙ x

  • and θ ∼ Cte.
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SLIDE 16

A Simple Model

To address the problem of the angle we need to go deeper in the model

x = − 1

2ρ(˙

x2 + ˙ z2)Sim(z) sin(θ + β)(Cl sin θ + Cd cos θ) M¨ z = −Mg + 1

2ρ(˙

x2 + ˙ z2)Sim(z) sin(θ + β)(Cl cos θ − Cd sin θ) Notice that: β = arctan −˙

z ˙ x

  • and θ ∼ Cte.
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SLIDE 17

Model expansion and simulation

Cd ≪ Cl ≃ 1

On water: (z < 0)

x = − 1

2ρ(˙

x2 + ˙ z2)Sim(z) sin(θ + β) sin θ M¨ z = −Mg + 1

2ρ(˙

x2 + ˙ z2)Sim(z) sin(θ + β) cos θ

On air: (z > 0)

x = 0 M¨ z = −Mg

Immersed Area

Sim =        R2

  • arccos
  • 1 − s

R

  • 1 − s

R

1 −

  • 1 − s

R

2

  • , z < 0 & |z| < 2R sin θ

πR2 z < 0 & |z| > 2R sin θ 0, z > 0

M = 0.1 kg ρ = 1 g/cm3 g = 9.8 m/s2 R = 0.025 m

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SLIDE 18

Simulation: Stone Position

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Simulation: Stone Position

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Simulation: Energy Loss

◮ We can try a little analytical trick:

∆E ≃ 1

2M ˙

x2

f − 1 2M ˙

x2

0 =

tcoll Fx ˙ xdt ≃ −1.4NMg2π

  • M sin θ

CρR

≃ −1.928 J But in the end the most precise result come from the model:

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SLIDE 21

Simulation: Best Angle

Angle With Water:

◮ ’Magic angle’

≃ 20o

◮ Best angle

≃ 15o

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SLIDE 22

Experiment 1 - Rosellini

Set up: Results:

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Experiment 1 - Rosellini

Set up: Results:

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Experiment 2 - Hewitt

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Contests and curiosities

A little bit of history

◮ Record of stone skipping as a sport goes back at least to 1583. ◮ Tradition holds that the sport was begun by an English king

who skipped stones across the Thames.

◮ Nowadays there are tens of tournaments and championships

  • n stone skipping.

Stones manufactured for skipping

The current record for stone skipping is Russ Byars with a throw of 51 skips.

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SLIDE 26

Feeling Lucky?

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51 skips

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Simulation: Mass

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Simulation: Radius