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Title: Physical oceanography, tides and coastal flooding the science behind it all


1
Physical oceanography, tides and coastal flooding
the science behind it all
  • Dr Kevin Horsburgh
  • Head of the National Tidal and Sea Level Facility
  • Physics Teachers Conference
  • 26 June 2008

2
Proudman Oceanographic Laboratory
  • Is a component laboratory of the Natural
    Environment Research Council (NERC), and is based
    in Liverpool
  • In partnership with the Met Office, we supply the
    coastal flood forecasts that are used
    operationally for the UK
  • POL science helps develop improved coastal
    forecasting systems
  • Sea level research
  • Shelf sea physics
  • Statistics of extremes
  • Effect of climate change on extreme sea level
    events
  • Wave modelling wave climate research
  • Real-time monitoring

3
Outline
  • Context coastal flood forecasting, operational
    oceanography, real-time marine monitoring
  • Physics underlying some key oceanographic
    phenomena
  • Forecasting models
  • Climate change and its implications
  • Sea level rise
  • Importance of observations (empiricism)

4
  • Insurance companies pay about 1 billion annually
    due to coastal flooding
  • Without sea defences this figure would rise to
    3.5 billion
  • Defences costly! New sea wall at Blackpool cost
    60 m

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  • Increased flooding due to sea level rise, or
    larger storm surges and waves due to increased
    storminess, could impact on economic and social
    systems, as well as fragile ecosystems
  • An important tool in the management of episodic
    flood events is a reliable forecasting capability
  • Improved operational models lead to better risk
    management, and inform high-level policy
    decisions

10
North Sea storm surge of 1953
Sea Palling, Norfolk (1 Feb 1953)
Oosterscheldekering (part of Delta works)
Thames Barrier (1987- )
11
Components of the UK coastal flood warning system
12
Tides
  • Tides are one of the most important dynamical
    phenomena in continental shelf seas
  • The earliest evidence of knowledge of tidal
    motion dates back to the Indian Vedic period
    (1500 BC)
  • The scientific civilizations of the Mediterranean
    didnt know much about the tide we now know
    that this is because the Mediterranean basin
    responds only slightly to the tide generating
    forces
  • The English monk Bede was aware of tidal
    behaviour around the Northumbrian coast in 730 AD
  • Steps towards a proper understanding of tides
    were taken by European scientists in the 16th and
    17th centuries. The key physical law is the Law
    of Universal Gravitation (Newton, 1687)

13
The equilibrium tide
  • The notion of a tidal bulge of water aligned with
    tidal forces- the equilibrium tide was
    suggested by Newton
  • The gravitational pull of the Sun is only 0.46
    that of the moon
  • Every fortnight, when the moon is full or new,
    the solar and lunar tides combine to give spring
    tides
  • The behaviour of the real ocean is far more
    complicated than this due to land masses,
    friction and inertia

14
The harmonic method of prediction
  • Practical methods of tide prediction are based on
    the principle (Laplace, 1755) that, for every
    frequency in the equilibrium tide there exits a
    constituent in the real tide with the same
    frequency
  • Harmonic analysis finds the amplitude (size) and
    phase (timing) of each constituent
  • The tide at any place is the sum of a large
    number of constituents, each of which is
    associated with a distinct (usually astronomical)
    cause
  • Tide tables were first produced by precision
    mechanical machines, but are nowadays computed
    rapidly by computer

15
Storm surges
  • Deviations from predicted tidal heights are
    (largely) due to meteorological effects. A storm
    surge is the effect of the weather on the sea
    surface due to
  • atmospheric pressure
  • wind stress
  • A surge is defined as
  • Height of observed sea level - height of
    predicted tide
  • Statistical analysis at UK ports shows that tidal
    predictions give
  • 90 of HW height to within 20 cm
  • 95 of HW times to within 10 minutes
  • Residuals (surge) gt 50 cm occur 10 times per
    year

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Images from Katrina
Levee overtopping Bay St Louis
H90,Gulfport, FL
18
Surges in Bangladesh
Notable storm surges impacting the coast of
Bangladesh since 1974
Cyclone 02B April 1991
  • November 1970 300,000 fatalities
  • April 1991 138,000 fatalities

19
Dynamics of storm surges
  • The response of the sea surface to atmospheric
    pressure can be estimated from the so-called
    inverted barometer effect
  • A change in atmospheric pressure of 1 mb
    corresponds to a rise in sea level of about 1 cm.
    During an extreme low, sea level can rise in
    places by up to 0.5 m due to pressure alone
  • Sea level rise due to wind effect is inversely
    proportional to the depth. The wind effect is
    most severe in shallow water
  • With some typical values for strong winds, sea
    level rise in the southern North Sea due to wind
    alone is 1.5-2.5m

20
The equations of motion for fluids
  • a.k.a. the momentum equations, the dynamical
    equations or (incorrectly) the Navier-Stokes
    equation.
  • Newtons 2nd Law a F/m
  • If m 1 (unit mass), then the acceleration on
    this 1 kg parcel of water is simply the sum of
    forces acting on it
  • From this simple beginning, some rather complex
    equations can be derived that describe the flow
    of fluids on a rotating Earth
  • In the vertical, a simplification leads to the
    hydrostatic approximation
  • The oceanographic pressure field is usually in
    hydrostatic balance, but there are exceptions
    (e.g. upwelling, convective overturning, deep
    water formation)

21
Alternative forms of these equations
  • In the most general case, the friction terms are
    written as gradients of stress
  • In real flows, these stresses are the Reynolds
    stresses, and viscous stress due to the fluids
    molecular viscosity can be ignored. The equation
    for the mean flow is then
  • Finally, we may choose to parameterise the
    Reynolds stresses using an eddy viscosity
    coefficient and the velocity shear of the main
    flow (by analogy with viscous stress in a
    Newtonian fluid)

F ma
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The Coriolis force
  • Newtons Laws apply to an inertial frame of
    reference (subject to no acceleration - fixed
    relative to distant stars).
  • Transformation to rotating axes gives rise to an
    apparent force called the Coriolis force which
    causes a deflection to the right of motion in the
    northern hemisphere, and to the left of motion in
    the southern hemisphere (cum sole).
  • In the northern hemisphere, northwards movement
    (positive v) contributes acceleration towards the
    east.
  • f is called the Coriolis parameter and f 2?
    sin? where ? is the Earths angular rotation
    rate (7.29 x 10-5 rad s-1) and ? is latitude.
    Hence f is maximum at the poles but zero at the
    equator.

24
Simple demonstration of the Coriolis force
  • Imagine a cannon at the north pole, firing at a
    target to the south. The missile moves in a
    straight line in an inertial frame (obeys
    Newtons 1st Law). The target is moving eastward
    as Earth spins, and the shot appears to veer to
    the right
  • Earths spin is a vector quantity. Just like
    velocity it can be resolved into component
    directions. In this case, spin about Earths axis
    is broken up into spin in the local horizontal
    plane and spin normal to this (a rolling action)
  • At the poles, all of Earths spin O is in the
    local horizontal plane (around the local vertical
    axis). At the equator, none of it is.

North
?
25
Geostrophic flow
  • If the flow is steady (i.e. no accelerations) and
    frictional forces can be neglected then the only
    terms in the equations of motion are the pressure
    gradient and the Coriolis force. This is called
    geostrophic balance
  • The geostrophic flow is at right angles to the
    pressure gradient. A good example of geostrophic
    flow is the wind above the atmospheric boundary
    layer (where friction is negligible)
  • The Gulf Stream is also in geostrophic balance to
    a good approximation, with a sea surface slope
    balancing a geostrophic current. This is
    expressed by the gradient equation, fv g tan?

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North Sea storm surge of 9 November 2007
28
Synoptic situation on Friday 9 November 2007
29
Real-time data operational model performance
Immingham
Lowestoft
Sheerness
30
Clean-up begins after the typhoon that never
wasBy DAVID DERBYSHIRE
  • Seawalls were breached at Walcott in Norfolk
  • Sea levels around Lowestoft were about 0.7m below
    defences
  • Some overtopping around Great Yarmouth

31
Comparison with 1 February 1953
32
Architecture of the ensemble surge system
33
Output from the MOGREPS ensemble surge suite
18Z run on 8/11/08
34
Spatial difference between extreme ensemble
member and deterministic forecast
35
  • On this occasion there was no significant change
    in inundation with the extreme member
  • Topography exposes all low-lying areas to risk at
    moderate extreme levels.
  • Wherever local topography implies a series of
    critical threshold levels, inundation mapping can
    set multiple warning levels which the ensemble
    system can then target probabalistically

36
IPCC WG1 of 4AR (February 2007)
37
Effects of climate change on coastal sea level
  • When water depth changes, and when also there are
    coupled changes in regional meteorology, there
    will be changes in storm surges, tides, waves and
    extreme water levels
  • Most records show evidence for rising mean sea
    levels (MSL) during the past century
  • IPCC Fourth Assessment Report (Summary for
    Policymakers) concluded that there has been
    global MSL rise of
  • 1.8 ( 0.5) mm/year from tide gauge data
    (1961-2003)
  • 3.1 ( 0.7) mm/year from satellite altimetry
    (1993-2003)
  • Latest predictions for the decade 2090-2099 from
    a range of numerical models, and excluding rapid
    changes in ice flow, advise a MSL rise of 20-60cm
  • These rates will be regionally different due to
    ocean circulations and regional land movements

38
Ensemble projections of change in extreme sea
levels
Uncertainty in large scale atmospheric forcing
Run surge model simulations to estimate
uncertainty range in local extreme water levels
39
  • Annual maximum skew surges and 50-year return
    levels with time-trend (from 5 largest per year)

40
MSL Changes in Last 100 Years
Is the rate of rise increasing ? Not clear. On
basis of 20th century tide gauge data alone. Yes.
On basis of altimeter data from the 1990s.
But there is large decadal variability in
all geophysical signals
41
Tools for Measuring Sea Level Changes
Tide Gauges Satellite Altimetry
Sea Floor Systems
42
The UK National Tide Gauge Network
43
Geodetic Tools for Measuring Land Level Changes
GPS
Absolute Gravity

44
Current measurement the Acoustic Doppler
Current Profiler (A.D.C.P.)
  • Measures currents at all depths by emitting
    acoustic pulses and determining the Doppler shift
    of the return signal reflected by passive
    particles
  • ADCPs can be vessel-mounted (looking down), or
    placed on the bed (looking upwards) in a
    recoverable frame.
  • The Doppler effect. When an acoustic signal of
    frequency f0 is reflected by a target moving
    relative to the source/receiver, at relative
    speed V, the backscattered signal is frequency
    shifted by an amount ?f 2f0V / c (c
    speed of sound)
  • To derive velocity components in the x, y, z
    coordinate directions required, ADCPs have four
    acoustic beams

45
Measurement of suspended particulates
Path length
  • Suspended particulate material (S.P.M.) can be
    measured with an optical beam transmissometer.
    The attenuation of a beam of light over a known
    path length can be accurately related to S.P.M.
    concentrations (as low as 1 mg/l).
  • A 660 nm light source (rapidly absorbed in
    seawater) ensures that sunlight does not
    contaminate the received signal, and eliminates
    attenuation due to gelbstoff.

46
Biological measurements - fluorometers
  • Fluorometers use the principle of fluorescence to
    estimate the amount of chlorophyll in a volume of
    water.
  • Chlorophyll (and other fluorescent materials),
    when excited by a source of light, absorb light
    in one region of the visible spectrum and then
    re-emit a portion of the energy at longer
    wavelengths.
  • Chlorophyll is excited by blue light at 455 nm
    and re-emits red light at 685 nm.

455 nm
685 nm
47
  • The small amount of red light produced by the
    blue light source is blocked by a suitable
    filter, as is any scattered blue light reaching
    the detector.
  • A detector (photo-diode) measures the amount of
    fluorescent light emitted
  • The estimated concentration of chlorophyll can be
    used as an indicator of phytoplankton biomass.
  • Optical properties of phytoplankton are functions
    of size, shape, species and phytoplankton health!

Blue LED
Red-removing filter
Blue-removing filter
48
Concluding remarks
  • Oceanography is a physical science, and is
    replete with fundamental physics
  • Classical mechanics is at the heart of the
    complex computer models used for predicting
    coastal flooding, ocean currents, meteorology and
    climate change
  • By refining such models we can provide effective
    coastal flood warning that is so essential to
    protect lives, property and infrastructure
  • Uncertainties remain in any forecasting system.
    Their quantification through ensemble forecasting
    and statistical methods is a subject of much
    current research
  • All models need validation with accurate,
    repeatable observations. Observation is the
    bedrock of science.
  • The precision instrumentation of the
    oceanographer makes use of hydrostatics, optics,
    Doppler effect, electronics, gravity and many
    aspects of the electromagnetic spectrum
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