Transcript Document

Shallow Water Waves: Tsunamis and Tides
MAST-602 Lecture Oct.-14, 2008 (Andreas Muenchow)
Knauss (1997):
p. 218-222 (tsunamis and seiches)
p. 234-244 tides
p. 223-226 Kelvin waves
Descriptions: Tsunamis, tides, bores
Tide Generating Force
Equilibrium tide
Co-oscillating basins
Tsunamis:
… shallow water gravity waves with a continuum of
periods from minutes to hours that all propagate at a
phase speed of c=(gH)1/2
… forced by earth quakes and land slides
Dec.-26, 2004 Sumatra tsunami:
deadliest natural disaster,
225,000 people killed,
30-m high wave
o
Seychelles
Sealevel of Seychelles. Data from the
Seychelles Meteorological Office.
Tsunamis:
… shallow water gravity waves with a continuum
of periods from minutes to hours that all propagate
at a phase speed of c=(gH)1/2
… forced by earth quakes and land slides
Tides:
… shallow water gravity waves with generally discrete
periods near 12 hours (semi-diurnal) and 24 hours
(diurnal) that all propagate at phase speeds c=(gH)1/2
… forced by periodicities of the sun-moon-earth orbits
… like all waves, they can break
(tidal bore movie)
Tides
High or low?
Tides
High it was:
Nova Scotia,
Canada
Tidal Wave Forms: Why do they all look different?
Semi-diurnal
Diurnal
Mixed
Mixed
Tidal Sealevel Amplitude (color) and Phase (white contors)
for the lunar semi-diurnal M2 constituent (T=12.42 hours)
Tidal Currents:
Observations
Predictions
Frequency (cycles/day)
Muenchow and Melling 2008)
in review
What’s wrong with this picture?
Tide Generating Force is the vector sum of:
1. Gravitational force exerted by the moon on the earth;
2. Centrifugal force (inertia) of the revolution about the
common center of mass of the earth-moon system.
What’s wrong with this picture?
>gravity
> inertia
Tide Generating Force is the vector sum of:
1. Gravitational force exerted by the moon on the earth;
2. Centrifugal force (inertia) of the revolution about the
common center of mass of the earth-moon system.
Centripetal and Centrifugal forces
Centripetal force is the actual force
that keeps the ball “tethered:”
“string” can be gravitational force
Centrifugal force is the pseudoforce (apparent force) that one
feels due to lack of awareness
that the coordinate system is
rotating or curving (inertia)
centrifugal acceleration = 2R
Revolution with
Rotation
Revolution without
Rotation
Moon around Earth
(“dark” side of the moon):
R is not constant on the surface
Earth around Sun
(summer/winter cycles):
R is constant on the surface
centrifugal acceleration = 2R
© 2000 M.Tomczak
Particles revolve around the
center of gravity of the
earth/moon system
All particles revolve around this center
of gravity without rotation …
… and execute circular motion
with the same radius R
 centrifugal force the same
everywhere
Revolution without rotation
All particles revolve around this
center of gravity without rotation
…
… and execute circular motion
with the same radius R
 centrifugal force the same
everywhere
Centrifugal acceleration same everywhere on the surface of earth
but, gravitational acceleration is NOT because of distance r:
Force of gravity between two masses
M and m that are a distance r apart
Sun
or
Moon
© 1996-1999 M. Tomczak
Tide Generating Force = Gravity-Centrifugal Force
Local vertical component:
Local horizontal component:
1 part in 9,000,000 of g
all that matters
Horizontal tide generating force (hTGF) moves waters around
Equilibrium Tide: Diurnal Inequality
h(t)=cos(w1t)+cos(w2t)
w1=2p/12.42 (M2)
w2=2p/23.93 (K1)
h(t)=A*cos(w1t)+B*cos(w2t)
w1=2p/12.42 (M2)
w2=2p/23.93 (K1)
A>B
semi-diurnal
A~B
mixed
A<B
diurnal
Tidal Wave Forms: Diurnal inequality plus spring/neap cycles
Semi-diurnal
Diurnal
Mixed
Mixed
Sun’s tide-generating force (hTGF) is 46% of the moon’s hTGF
hTGF=
= mass/r3
Equilibrium Tide: Spring/Neap cycles
h(t)=cos(w1t)+cos(w2t)
w1=2p/12.42 (M2)
w2=2p/12.00 (S2)
Red: sun’s bulge
Grey: moon’s bulge
Blue: rotating earth
Dials:
1 lunar month (29 days, outer dial)
1 solar day (24 hours, inner dial)
Equilibrium Tide: Other periodicities, e.g., lunar declination
Equilibrium tide: Other periodicities
Orbital planes
all change
declinations
slowly
Homework ---> head to Australia
Basic Exercises in Physical Oceanography
Exercise 5: Tides
Prof. Mathias Tomczak
http://www.es.flinders.edu.au/~mattom/IntExerc/basic5/
Currents
Sealevel
Time
Kelvin wave propagation
In the North Sea
© 1996 M. Tomczak