02. partial standing wave

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Page 1: 02. Partial Standing Wave
Page 2: 02. Partial Standing Wave

Capsizing of Ships

Following sea is the most dangerous!

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Q#5: Perfect Standing WaveQ#5: Perfect Standing Wave(Reflection from vertical wall)(Reflection from vertical wall)

cos( ) cos( )A kx t A kx t

2 cosh ( ) cos sincosh

gA k z h kx tkh

( )kze deep

Total Pressure

,u wx z

p gzt

Page 5: 02. Partial Standing Wave

Partial Standing Wave

cos( ) cos( )2 2( )cos ( )sin

( ) cos cos( )2 2where

( ) sin sin( )2 2

i r

i r

i r

H Hkx t kx t

I x t F x tH HI x kx kx

H HF x kx kx

2 2

( )Max/Min when 0 tan( )

cos(2 )2 2 2i i rr

F xtt I x

H H HH kx

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max

min

max min

max min

max min

1At quasi-antinode : ( )21At quasi-node : ( )2

distance between and 4

Reflection coefficient

i r

i r

i

r

r

i

H H

H H

L

HH

HH

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Typical Size of LNG Tank

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Seiching

Long-period oscillation of harbors due to resonance sloshing

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[1] (24%) Select proper answer   When celerity depends on wave length, the wave is

called (dispersive wave, non-dispersive wave).   With (dispersive wave, non-dispersive wave),

communication is possible.   Acoustic waves are (dispersive waves, non-dispersive

waves).   Wave induced dynamic pressure is (linearly,

quadratically) proportional to wave height.   When the distance between semi-antinode and semi

node of a partial standing wave is 30m, the wavelength of the incident wave is (120m, 60m)

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(Longer, Shorter) water waves travel faster in deep water.   The front of water waves in deep water moves with (celerity,

group velocity).   The primary restoring force for water waves of wavelength=20-

200m is (gravity, Coriolis, surface tension) force.   The wave energy is (linearly, quadratically) proportional to wave

height.   Long waves generated by large-scale atmospheric pressure

variation are called (tidal waves, tsunamis, storm surge)   The maximum vertical acceleration of water-wave particles occurs

at (crest, crossing point)   Water depth=200m is considered to be (deep, transitional) for a

sinusoidal water wave of wavelength=470m.  

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[2] (6%) When a hypothetical sinusoidal wave satisfies the dispersion relation ω²=2k² between circular frequency ω and wave number k, find its celerity and group velocity.

  [3] (4%) When the potential energy of a

regular wave for certain area is 20000J, what is the corresponding kinetic energy?

  [4] (6%) The group velocity of a shallow

water wave is 3m/s. What is the corresponding water depth?

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[5] Consider a deep-water wave with 8-s period and 4-m height?

(a) (10%) What is the power of this wave along the crest width of 500m?

(b) (10%) If this deepwater wave propagates to the area of 2-m water depth, what is the new wave length and wave height at that location? (Assume 2D wave of normal incidence, shallow-water wave at 2-m depth, and mild bottom slope: use conservation of wave energy flux (power))

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[6] (a) (5%) When wave length is 100m at 10-m water depth, what is the corresponding wave period?

(b) (10%) When wave height=2m, what is the major semi-axis of the elliptical particle trajectory at z=-3m?

(c) (10%) What is the amplitude of the horizontal particle velocity at the same location z=-3m?

(d) (15%) If a vertical wall is present at the 10-m depth, a perfect standing wave will be formed in front of the wall. In that case, what is the dynamic pressure amplitude of the standing wave at z=-3m under the anti-node.

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Wave Refraction

Change of wave heading due to bottom topography

Cf. reflection, diffraction

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Refraction : change of wave direction due to bottom topography

0 10 1

0 0

1 1

0 10 1

0 0

1 1

from geometry

sin , sin. .

sin find new headingsin

cos , cos. .

cos find new Bcos

c t c tDiag Diag

c ac a

B BDiag Diag

B aB a

< Snell’s law >

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Combined shoaling & Refraction

2 20 0 0

0 0

0

reflectionIf negligible

diffractionPower(Energyflux) Conservation

1 12 2

shoaling coefficientwhere

= refraction coefficient

Normal Incidence no refracti

g g

gs r

g

s

r

gA B C gA B C

C BA K KA C B

KK

on

Oblique Incidence refraction occurs!

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Wave Breaker Type

Spilling: steeper crest : loose stability at cusp: mild beach slope

Plunging: overturning: steeper beach

Surging: bottom part surges over high-sloped beach: very steep beach=high reflection

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Plunging Breaking Waves

Waves break when the crest particle velocity exceeds its celerity.

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Wave Breaking

Deep & transitional depth:General: H/L=(1/7)tanh khDeep: H/L=1/7=0.14

Shallow McCowan’s criterion: flat bottomH=0.78hGoda-Weggel chart: with slope

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Wave Breaker Ex.) SPM 2-135

Given: Ho=2m, T=10s, beach slope=1/20, Kr=1.05

Find: breaker height Hb, depth hb, type by using Goda-Weggel chart

Unrefracted deepwater height: Ho’=Kr*Ho

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Unrefracted deepwater height: Ho’=Kr*Ho =2.1mHo’/GT²=0.00214From fig.2-72(m=0.05): Hb=3.15m; plunging

Hb/Ho’=1.5 & Hb/GT=0.0032From fig.2-73hb/Hb=0.96 therefore hb=3.02m

Surf-zone length=3.02/0.05=60m

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Wave breaking (20pt)

Deepwater T=8s, H=2m (Normal Incidence); beach slope=1/20

Find breaker height, breaker depth, and breaker type using the chart

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Wave-theory Selection Diagram

Water depth=1m, wave period=7s, wave height=0.3 m

Find the best wave theory

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Wave Kinematics

)sin(sinh)(sinh

tkxkdzdk

TH

w

)(2cos)(4sinh

)(2cosh2

163)cos(

cosh)(cosh

2tkx

kd

zdkkHtkxkdzdkgkHu

)cos(sinh

)(cosh tkxkdzdk

THu

)(4sinh

)(2sin)(2sinh2

163

)sin(cosh)(sinh

2 kd

tkxzdkkHtkxkd

zdkgkHw

Linear Wave KinematicsLinear Wave Kinematics

Stokes 2Stokes 2ndnd-order Wave Kinematics-order Wave Kinematics

tuax

tw

az

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3/27 SNAME Offshore Sym

Rec. Center (Garden Room)9:00 – 3:00

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2010 OCEN300 MINI-TERM PROJECT

Research on Ocean Hydro-Power

Team (5-member) selects a research topic related to ocean wave energy and tidal/current energy conversion.

Select a particular concept/system and describe how it works.

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Discuss pros and cons compared with other existing concepts.

Discuss its efficiency, survivability, and environmental impacts

Discuss the estimated cost when realized as a proto-type system.

Discuss the ideas how the existing technology and cost-effectiveness can be improved.

Prepare a 5-page report summarizing the study. (Report due on 5/4)

Prepare a team presentation. (Schedule: 4/29 A-E; 5/4)

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A: Allahar Jacquelene, Babbitt Charles, Blackburn Megan, Blackmar Philip, Brotzman Duncan

B: Brzezniak Michael, Cantu Felix, Castro Adrian, Dailey David, Demmer Michael

C: Feldman Kyle, Fields Waylon, Finkelshteyn Michael, Fisher Ian, Fluitt Timothy

D: Ford Bryce, Forester Aaron, Freyman Michael, Galatas Joel, Gibson Allison

E: Goebel Kevin, Gonzales Stephanie, Grant Alexander, Holub Chase, Hulsey Jennifer

F: Keel Ryan, Knoll Alex, Lee Sangwook, Lindanger Christopher, McBee Harvey

G: McClung Evan, McNeil Ryan, Medellin Abel, Messina Michael, Mieras Ryan

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H: Novasad Nicholas, Outten Kyle, Parker Christopher, Ramsey Paul, Ryan Christopher

I: States William, Stevenson Katy, Tallichet Jules, Thi Andy J: Tipton Craig, Vittone Cynthia, Walsh Andrew, Oyenike

Olaniyi

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Wave diffraction: wave deformation by structures

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Stokes’ 2nd-order Wave Theory

η= +

Valid when Ursell #: LH/h< 26.3

cos( )A kx t 21 cos(2 2 )2kA kx t

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Geometric Comparison

Nonlinear waves

higher and sharper crests

Shallower and flatter troughs

large steepness H/L (Linear theory assumes small amplitude)

Opened Orbit: Stokes’ drift

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WAVE-CURRENT INTERACTION

Wave in Coplanar CurrentH smaller, L longer: wave steepness

decreased, C faster

Wave in Adverse CurrentH larger, L shorter: wave steepness

increased, C slower

If adverse-current velocity > 0.5C: breaking

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Long waves

Tsunami Storm surge Tide

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Tsunami

Long-period (tens of minutes) gravity waves generated by submarine earthquakes, landslides, volcano eruptions, explosion, asteroid impact

Can build up heights in coastal regions as large as 30m

(ex. Hilo, Hawaii: 11m, Wavelength: can be as large as 200km)

Typical speed:Deep: speed of airplane (e.g. 500miles/hr)Coastal: speed of car (e.g.70 miles/hr)

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Tsunami

Magnitude of Earthquake Richter Scale M=log(A/Ao)(A: max. amplitude recorded by a seismograph

at 100km from epi-center, Ao=0.001mm)

Tsunami Magnitude m=2.61M-18.44M=7, m=0(Hmax=1m): small damageM=8, m=2.4(Hmax=10m)M>8.6, m>4(Hmax=30m): considerable damage

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Before 2004 Dec. 26 Tsunami

After December 26 Tsunami

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Storm Surge

Suction effects by large-scale low atmospheric pressure

Wave/water-mass pile up at costal region by strong winds

Max. anomaly=f(max. wind vel., wind direction, lowest atmospheric pressure)

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Storm surge

Although the wind shear stress is usually small, its effect, when integrated over a large body of water, can be catastrophic.

Hurricanes, blowing over the shallow continental shelf of GOM, have caused rises in water levels in excess of 6m at the coast.

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Empirical storm-surge forecasting

Max anomaly (sea-rise in cm)=a P + b V² cos D

a=0.99 cm/mbb=0.048(baylength(km)/ bay

meandepth(m))V=max wind velocity (m/s)P=(spatial mean – lowest) atmospheric

pressureD=wind direction

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Empirical Storm-surge Forecasting EX

Find the maximum sea-rise when

Lowest atm pressure=0.85 barSpatial mean atm pressure=1 barBay length=5kmBay mean depth=5mMax wind velocity=50m/sNormal wind direction

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Tidal Wave: sun-moon-earth gravitation

Semi-diurnal tide: 2 highs & 2 lows/day (ex Cape-Cod)

Diurnal tide: 1 high & 1 low/day (ex New Orleans)

Mixed tide: combination 1 semi-high and 1 major high – (ex Los Angeles)

Tidal Current: Ex. 3.1m/s (San Francisco) max=5.2m/s NOS (National Ocean Survey)

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Tidal Energy (7)

Promising West Coast Sites

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Tidal Energy (3) 21st Century projects

under consideration are based on ‘in stream turbine’ technology at sites with high tidal current velocities

Only a limited number of suitable sites in continental USA with San Francisco the best

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Current Energy Conversion

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Tidal Energy Conversion

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Tidal Energy (2)

La Rance dam and typical turbine/generator configuration

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http://www.youtube.com/watch?v=ZcA3e8_j8XA

http://www.youtube.com/watch?v=rQtMPdLZ2L4&NR=1

http://www.youtube.com/watch?v=94iZa96HpUA

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Tidal Energy

http://www.youtube.com/watch?v=tSBACzRE3Gw&feature=related

http://www.youtube.com/watch?v=4Iq-h4ShZ8s&feature=related

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Have a Good Spring Break!

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WOW (Waves On Web)

Ceprofs.tamu.edu/mhkim/wow

cavity.ce.utexas.edu/kinnas/wow/public_html/waveroom

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Wavemaker: Review

Flap motion: 1.5 cycles/s, h=80cm, H=3cm Find T=?, L=?, C=?, k=?, w=?, Cg=?, Power(tank

width=90cm)=? Breaking? Speed of wave front=? max horizontal particle velocity? max radius of particle orbit? Total max pressure 10cm below MWL?

Mild-slope (m=0.05) is installedH & L at h=4cm? C=? Cg=? Will it break? What

type? Length of surf-zone? Which wave theory?