physics of surfing energy - satellite geodesy at the ...topex.ucsd.edu/ps/energy.pdf · physics of...

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Physics of Surfing Energetics of a Surfer David T. Sandwell (http://topex.ucsd.edu) Four styles of surfing • Waves Big swell coming? (storms) What makes “sets”? (dispersion) Why is Blacks Beach good for surfing? (refraction) Riding waves “catching” the wave (speed) “dropping-in” (energy conservation) “tube riding” (tapping wave energy) “need more speed” (surfboard drag) 1 2 kg 1 kg Which ball is going faster when it reaches the bottom? (a) (b)

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Page 1: physics of surfing energy - Satellite Geodesy at the ...topex.ucsd.edu/ps/energy.pdf · Physics of SurÞng Energetics of a Surfer David T. Sandwell () ¥Four styles of surÞng ¥Waves

Physics of Surfing

Energetics of a SurferDavid T. Sandwell

(http://topex.ucsd.edu)

• Four styles of surfing

• Waves– Big swell coming? (storms)

– What makes “sets”? (dispersion)

– Why is Blacks Beach good for surfing?(refraction)

• Riding waves– “catching” the wave (speed)

– “dropping-in” (energy conservation)

– “tube riding” (tapping wave energy)

– “need more speed” (surfboard drag)

1 2 kg 1 kg

Which ball is going faster when it reaches the bottom?

(a) (b)

Page 2: physics of surfing energy - Satellite Geodesy at the ...topex.ucsd.edu/ps/energy.pdf · Physics of SurÞng Energetics of a Surfer David T. Sandwell () ¥Four styles of surÞng ¥Waves

Which ball is going faster when it reaches the bottom?

(a) (b) (c)

conservation of energy(assume no friction)

kinetic energy + potential energy = constant

mgH =1

2mv

2m

m

v

H

mv

Page 3: physics of surfing energy - Satellite Geodesy at the ...topex.ucsd.edu/ps/energy.pdf · Physics of SurÞng Energetics of a Surfer David T. Sandwell () ¥Four styles of surÞng ¥Waves

optimal skateboard ramp(The brachistochrone problem)

What is the best ramp shape for the minimum time down?

Page 4: physics of surfing energy - Satellite Geodesy at the ...topex.ucsd.edu/ps/energy.pdf · Physics of SurÞng Energetics of a Surfer David T. Sandwell () ¥Four styles of surÞng ¥Waves
Page 5: physics of surfing energy - Satellite Geodesy at the ...topex.ucsd.edu/ps/energy.pdf · Physics of SurÞng Energetics of a Surfer David T. Sandwell () ¥Four styles of surÞng ¥Waves

60 ft

35 mph

24 ft

22 mph15 ft

18 mph4.5 ft

10 mph

ocean depth and breaker height - empirical

Hb - height of breaker

db - depth where wave

breaks

db

=1.28Hb

Page 6: physics of surfing energy - Satellite Geodesy at the ...topex.ucsd.edu/ps/energy.pdf · Physics of SurÞng Energetics of a Surfer David T. Sandwell () ¥Four styles of surÞng ¥Waves

Mavericks video

shallow water waves

cs = gd

Page 7: physics of surfing energy - Satellite Geodesy at the ...topex.ucsd.edu/ps/energy.pdf · Physics of SurÞng Energetics of a Surfer David T. Sandwell () ¥Four styles of surÞng ¥Waves
Page 8: physics of surfing energy - Satellite Geodesy at the ...topex.ucsd.edu/ps/energy.pdf · Physics of SurÞng Energetics of a Surfer David T. Sandwell () ¥Four styles of surÞng ¥Waves

breaking waves

db

surfers

empirical relation

Hb - height of breaker

db - depth where wave

breaks�

db

=1.28Hb

Page 9: physics of surfing energy - Satellite Geodesy at the ...topex.ucsd.edu/ps/energy.pdf · Physics of SurÞng Energetics of a Surfer David T. Sandwell () ¥Four styles of surÞng ¥Waves

“catching the wave”

db

surfers

paddle speed

Hb - height of breaker

db - depth where wave

breaks�

cb = 1.28gHb

paddle speed <= wave speed

60 ft

35 mph

24 ft

22 mph15 ft

18 mph4.5 ft

10 mph

Page 10: physics of surfing energy - Satellite Geodesy at the ...topex.ucsd.edu/ps/energy.pdf · Physics of SurÞng Energetics of a Surfer David T. Sandwell () ¥Four styles of surÞng ¥Waves

“dropping in”

Hb

top of wave

bottom of wave

KEbottom = KEtop + PE

1

2mvd

2=1

2mcb

2+ mgHb

vd2

= cb2

+ 2gHb = 3.28gHb

g - acc. Gravity

cb - wave speed

vd - surfer speed after drop

“dropping in”

59.827.217.023tow-in

35.216.010.08tube

27.912.77.95fun

15.26.94.3 1.5longboard

vd

(mph)

vd

(m/s)

cb

(m/s)

Hb

(m)

style

Page 11: physics of surfing energy - Satellite Geodesy at the ...topex.ucsd.edu/ps/energy.pdf · Physics of SurÞng Energetics of a Surfer David T. Sandwell () ¥Four styles of surÞng ¥Waves

correction for surfer height

H' Hb

H' = Hb - 1/2 Hs

effective height = breaker height - 1/2 surfer height

- overhead waves are good

- waist high waves are bad

- short surfers and heavy boards have an advantage in small waves

Pipeline video

dropping in

Page 12: physics of surfing energy - Satellite Geodesy at the ...topex.ucsd.edu/ps/energy.pdf · Physics of SurÞng Energetics of a Surfer David T. Sandwell () ¥Four styles of surÞng ¥Waves

“dropping in”

Hb

top of wave

bottom of wave

KEbottom = KEtop + PE

1

2mvd

2=1

2mcb

2+ mgHb

vd2

= cb2

+ 2gHb = 3.28gHb

g - acc. Gravity

cb - wave speed

vd - surfer speed after drop

“dropping in”

59.827.217.023tow-in

35.216.010.08tube

27.912.77.95fun

15.26.94.3 1.5longboard

vd

(mph)

vd

(m/s)

cb

(m/s)

Hb

(m)

style

Page 13: physics of surfing energy - Satellite Geodesy at the ...topex.ucsd.edu/ps/energy.pdf · Physics of SurÞng Energetics of a Surfer David T. Sandwell () ¥Four styles of surÞng ¥Waves

“cutting across”

back of wave

front of wave

vd !

cb

cb

2

vd

2=1.28

3.28= cos

2!

! =~ 50˚

top

view

This angle is independent of

wave height or wave speed!

Page 14: physics of surfing energy - Satellite Geodesy at the ...topex.ucsd.edu/ps/energy.pdf · Physics of SurÞng Energetics of a Surfer David T. Sandwell () ¥Four styles of surÞng ¥Waves

“riding the wave”

Suppose the surfer remains on the steepest part of the wave having

a slope s. What is the rate of potential energy increase supplied to

the surfer?

cb s

P ˙ E = sgcbside view

v(t)2

= vd2

+ sgcbo

t

! dt

v(t)2

= 3.28gHb + tsg 1.28gHb

How does speed increase

with time?

speed video

Page 15: physics of surfing energy - Satellite Geodesy at the ...topex.ucsd.edu/ps/energy.pdf · Physics of SurÞng Energetics of a Surfer David T. Sandwell () ¥Four styles of surÞng ¥Waves

“the drag”

v(t)2 = 3.28gHb + 1.13g

3 / 2 s Hb

1/ 2 t ! drag

total

velocity= paddle

drop in+ -slope of

“the curl”breaker

height

duration

of ride

energy

dissipation

Future Research

– Are the best surf spots in areas of narrow continental margin?

– Are “sets” real? What are the statistical properties of sets? Do “sets”become amplified when they reach shallow water?

– How does the shape of the bottom translate into the “perfect wave”?

– What is the terminal velocity for a given breaker height? (Can we establishthe magnitude of the drag term?)

– Need to instrument surfers with intertial sensors.