Physics of SurÞng Waves - part 2 · wave characteristics ¥generated by storms at sea ¥far from...

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Physics of Surfing Waves - part 2 David T. Sandwell (http://topex.ucsd.edu/ps) Physics of waves Characteristics of waves Generation of waves by storms Wave speed - shallow vs. deep ocean Sets - dispersion Refraction of waves - Why is Black!s so good? Exercises: April 15 (each problem is covered in class) 1. Derive the expression for the period of a harmonic oscillator with mass m and spring constant k. 2. Derive the expression for the speed of a deep water wave in terms of the wave period T. 3. What are sinh, cosh, and tanh in terms of the exponential function? What is tanh(10 -6 )? What is tanh(10)? 4. One more problem. Consider two waves of equal height but different period (T 1 =12.5 s and T 2 =13 s. What is the time between sets? Here is a hint: add two cosine functions h(t) = cos(! 1 *t) + cos(! 2 *t) where ! 1 = 2*" /T 1 ,use the trigonometric formula for the sum of two cosines, then interpret or plot the results.

Transcript of Physics of SurÞng Waves - part 2 · wave characteristics ¥generated by storms at sea ¥far from...

Page 1: Physics of SurÞng Waves - part 2 · wave characteristics ¥generated by storms at sea ¥far from the storm they are sinusoidal h x H A L h(x,t)=Asin 2!x L " 2!t T # $ % & ' ( c=

Physics of Surfing

Waves - part 2David T. Sandwell(http://topex.ucsd.edu/ps)

• Physics of waves

• Characteristics of waves

• Generation of waves by storms

• Wave speed - shallow vs. deep ocean

• Sets - dispersion

• Refraction of waves - Why is Black!s so good?

Exercises: April 15(each problem is covered in class)

1. Derive the expression for the period of a harmonic oscillator with mass mand spring constant k.

2. Derive the expression for the speed of a deep water wave in terms of thewave period T.

3. What are sinh, cosh, and tanh in terms of the exponential function? Whatis tanh(10-6)? What is tanh(10)?

4. One more problem. Consider two waves of equal height but differentperiod (T1=12.5 s and T2=13 s. What is the time between sets? Here is ahint: add two cosine functions h(t) = cos(!1*t) + cos(!2*t) where !1 = 2*"/T1 ,use the trigonometric formula for the sum of two cosines, theninterpret or plot the results.

Page 2: Physics of SurÞng Waves - part 2 · wave characteristics ¥generated by storms at sea ¥far from the storm they are sinusoidal h x H A L h(x,t)=Asin 2!x L " 2!t T # $ % & ' ( c=

wave characteristics

• generated by storms at sea

• far from the storm they are sinusoidal

h

xH

A

L

h(x, t) = Asin2!xL

"2!tT

#

$ %

&

' (

c =L

T phase velocity

L - wavelength

A - amplitude

H - height

T - period (5 - 18 s)

Page 3: Physics of SurÞng Waves - part 2 · wave characteristics ¥generated by storms at sea ¥far from the storm they are sinusoidal h x H A L h(x,t)=Asin 2!x L " 2!t T # $ % & ' ( c=

Airy solution

L - wavelength

g - acc. gravity

d - ocean depth

c(d) =gL

2!tanh

2!dL

"

# $

%

& '

(

) *

+

, -

1/ 2

deep water waves shallow water waves

d >> L /2

cd =gL

2!

d << L /2

cs = gd

What causes “sets”?

Page 4: Physics of SurÞng Waves - part 2 · wave characteristics ¥generated by storms at sea ¥far from the storm they are sinusoidal h x H A L h(x,t)=Asin 2!x L " 2!t T # $ % & ' ( c=
Page 5: Physics of SurÞng Waves - part 2 · wave characteristics ¥generated by storms at sea ¥far from the storm they are sinusoidal h x H A L h(x,t)=Asin 2!x L " 2!t T # $ % & ' ( c=

44 mph

60 mph

Munk theory of sets

D RSan Diego

Antarctic

storm

Waves arrive in San Diego at the same time t1.

Suppose the waves were generated at the same time to.

t1! t

o= 2R /c

1

t1! t

0= 2(R + D) /c

2

c2

= c1

R + D

R

"

# $

%

& '

c =gT

2! deep water dispersion

T2 = T1

R + D

R

"

# $

%

& '

Page 6: Physics of SurÞng Waves - part 2 · wave characteristics ¥generated by storms at sea ¥far from the storm they are sinusoidal h x H A L h(x,t)=Asin 2!x L " 2!t T # $ % & ' ( c=

Munk theory of sets

D RSan Diego

storm

h(t) = Acos2!tT1

"

# $

%

& ' + Bcos

2!tT2

"

# $

%

& ' , suppose B = A

h(t) = 2Acos !t1

T1

+1

T2

"

# $

%

& '

(

)

*

+

,

- cos !t1

T1

.1

T2

"

# $

%

& '

(

)

*

+

,

-

surf = mean period modulated by beat period

interval between sets

TB

= T1

1!R

R + D

"

# $

%

& '

!1

R = 7000 km D = 400 km T1

= 17s,

TB

= 5.5min

A long time to wait

between sets!

“sets”

D RSan Diego

Antarctic

storm

A=3 m, B=1m, sets every 5.5 min

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OCEANSIDE OFFSHORE, CA - Station:

04501

Water depth(m): 220.00

August 3, 2007

Average time between sets

8.8 min

cm

Page 8: Physics of SurÞng Waves - part 2 · wave characteristics ¥generated by storms at sea ¥far from the storm they are sinusoidal h x H A L h(x,t)=Asin 2!x L " 2!t T # $ % & ' ( c=

shallow water waves

cs = gd

Page 9: Physics of SurÞng Waves - part 2 · wave characteristics ¥generated by storms at sea ¥far from the storm they are sinusoidal h x H A L h(x,t)=Asin 2!x L " 2!t T # $ % & ' ( c=

wave refraction

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 10: Physics of SurÞng Waves - part 2 · wave characteristics ¥generated by storms at sea ¥far from the storm they are sinusoidal h x H A L h(x,t)=Asin 2!x L " 2!t T # $ % & ' ( c=
Page 11: Physics of SurÞng Waves - part 2 · wave characteristics ¥generated by storms at sea ¥far from the storm they are sinusoidal h x H A L h(x,t)=Asin 2!x L " 2!t T # $ % & ' ( c=
Page 12: Physics of SurÞng Waves - part 2 · wave characteristics ¥generated by storms at sea ¥far from the storm they are sinusoidal h x H A L h(x,t)=Asin 2!x L " 2!t T # $ % & ' ( c=
Page 13: Physics of SurÞng Waves - part 2 · wave characteristics ¥generated by storms at sea ¥far from the storm they are sinusoidal h x H A L h(x,t)=Asin 2!x L " 2!t T # $ % & ' ( c=

Conclusions

– Ocean waves: force of acceleration is balanced by the forceof gravity.

– Wind speed >= wave speed. 17-s period waves require windspeed of 27 m/s = 60 mph.

– Wave speed: d >> L/2 waves are dispersive; d << L/2 speeddepends on depth.

– Refraction is important when d < 5L.

Page 14: Physics of SurÞng Waves - part 2 · wave characteristics ¥generated by storms at sea ¥far from the storm they are sinusoidal h x H A L h(x,t)=Asin 2!x L " 2!t T # $ % & ' ( c=