Notes
Slide Show
Outline
1
Validation of Tsunami and Dambreak Hazard Models
  • Modelling SIG has adopted idea of using reference tests to establish the validity of modelling techniques
  • Reference tests should preferably be based on field or laboratory measurements
  • Where field data is sparse and of poor quality (as with tsunamis) need to include analytical models
  • These generally apply only in simplified situations, but these can often be matched in numerical  models
  • Where field and/or laboratory data available, what about experimental errors?
  • Experiments need authentication to identify possible measurement errors
  • Authentication can be established by eliminating obvious outliers, and by checks for mass conservation (e.g. masses under flow curves should balance)
  • A quick way of authentication is to fit a good numerical model: if there is agreement, then authentication and validation both happen together
  • If there is no agreement, then back to square 1!
  • Illustrate by two examples: An analytical tsunami validation and a laboratory dambreak validation
  • Propose for adoption by national standards authority for compliance testing
2
Tsunami Model Validation
  • Solitary wave analysis is known to describe the propagation of gravity waves (such as tsunamis) without a change of shape.
  • Can therefore run a model wave over some distance and check for change in shape
  • Can also check that wave speed is modelled correctly
  • This applies only in water of constant depth and negligible friction
  • These conditions are easy to arrange numerically by ensuring the constant wave depth is much larger than the wave height
  • The downstream boundary needs to be far enough away that no reflected waves interfere with the test.
  • Then only need a boundary condition describing the solitary wave
  • A 6m wave was chosen as this will reach about 10m against a fully reflecting (steep) coastline
  • This is a typical height for design investigations
  • 1000m depth chosen as this gives a wave speed of approximately 100m/s
3
Solitary Wave
  • See Ippen “Estuary and Coastline Hydrodynamics” p.122
  • η = wave height
  • H = peak height at x=Ct
  • h = normal water depth
  • C = wave speed ≈ [g(H+h)]1/2
  • Table at right shows η(t) for x=0, H=6m, h=1000m
  • Note: Wave tapered off from 0.133m at 60s to 0.0m at 0s to avoid an infinite wave length at infinitesimal heights.
4
Example: AULOS Results
  • For Accuracy Bias B = 7 (highest setting) the wave propagates over 60km without change in shape in a time between 600s (depth=1019m) and 605s (depth=1003m)
  • For Accuracy Bias B = 0 (default setting) the wave propagates at the same speed but with some numerical diffusion. This reduces the wave height.













  • Development of other standard tests for validation of modelling waves on sloping beaches now proposed for NZWERF research funding
5
Dambreak Model Validation: Experimental Layout
6
WES Test Flume (1960)
  • US Army Engineer  WES (Waterways Experimental Station), Vicksburg, Mississippi
  • Rectangular Flume 400ft (122m) long,   4ft (1.22m) wide
  • Slope = 0.005
  • Manning n = 0.009
  • Dam removal took 0.01-0.03s
  • Surface velocities measured by time lapse photography of floating confetti
  • Depths measured by timed photographs
7
Selection of Test Data
  • WES tested various combinations of dam breach openings and initial downstream base flows
  • Test 5.1 was chosen by Sanders (2001) for validation testing of his solution. This involved a full depth (0.3048m) rectangular breach of width 0.4 ft (0.122m).








  • The WES report does not picture the model dam for Test 5.1, but it was presumably similar to that for Test 6.1 (above), which differed only in having a narrower breach of width 0.24 ft (0.073m).
  • This shows the slot sides were defined by sharp edges, not rounded
8
Upstream Reservoir Levels
  • Levels at STA188
  • (57.3m from
  • upstream end)
  • Time(s)  Level(m)
  •       0          0.6096
  •       2          0.6066
  •       3          0.5944
  •       4          0.5971
  •       5          0.5944
  •       7          0.5913
  •     10          0.5913
  •     20          0.5913
  •     30          0.5913
  •     60          0.5852
  •   120          0.5547
  •   150          0.5425
  •   180          0.5304
9
Example: AULOS Results at STA188
  • Plotted STA188
  • results as per
  • previous table.


  • This suggests
  • that outflows are
  • accurately matched.


  • The model used the
  • energy equation at
  • the breach, with a
  • textbook discharge
  • coefficient CB=0.9
  • for sharp edges
  • (Henderson, 1966)


10
Downstream Observations
  • These were made at three points:
  • STA225, STA280, STA350
  • respectively 225, 280 and 350 ft
  • (68.6m, 85.3m and 106.7m) from
  • upstream end of flume.


  • Flow values calculated from
  • mean velocity x depth,
  • but only surface velocities available


  • Mean velocity V assumed = kVs
  • Where Vs is surface velocity


  • k was assumed to be 0.80 by WES,
  • but this is too low except at STA225.
  • Analytically, k=0.88 a better estimate for
  • smooth channels.
11
Example: AULOS Depth Results
  • The depth validation is
  • generally good, with
  • excellent matching of
  • wave front arrival times
12
Example: AULOS Flow Results
  • The validation again
  • gives an excellent
  • match with dambreak
  • wave arrival times,
  • but the flow match is
  • only within about 10%
  • at STA 225 (k too high)
  • and STA280 (k too low).


  •  The close match at
  •  STA350 and with
  •  reservoir drawdown
  • upstream (STA188)
  • suggests main problem
  • with evaluating k.
13
Conclusions
  • Reference tests are an excellent way to establish the validity of modelling techniques
  • They also indicate the effect of using various model tuning parameters
  • Where possible, reference tests should be based on field or laboratory measurements
  • Analytical models can partly fill the gap where field data is sparse or of poor quality (as with tsunamis)
  • For tsunamis, a solitary wave forms a good analytical test for the ability of a model to reproduce wave behaviour in deep water.
  • Further work on runup on sloping beaches will (hopefully) follow soon.
  • For dambreak waves, the 1960 WES laboratory experiments are a useful source of wave behaviour under a range of conditions.
  • Experimental scatter in level measurements can be averaged out
  • The evaluation of mean velocity from the measured surface velocity required appeal to mass conservation plus an analytical shear model
  • The result adjustments have been authenticated partly by successful fitting with a model which conserves mass, momentum and energy
  • All input data required for sample validation of numerical tsunami and dambreak models is documented in this presentation
  • These tests are therefore recommended as suitable for adoption by a national standards authority for compliance testing.