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Title: Application of modal analysis to strongly stratified lakes


1
Application of modal analysis to strongly
stratified lakes
Supervisor Jörg Imberger
  • PhD candidate Kenji Shimizu

2
Overview
Force
Currents
Energy flux
Turbulence
3
Objective Contents
Objective better understanding basin-scale
motions Methodology modal analysis
  • Modes? Modal analysis? Motivation
  • Horizontal structure excitation of internal
    waves gyres in Lake Biwa Numerical
    simulation
  • Energetics damping of internal waves in Lake
    Kinneret Field data
  • Damping mechanisms of internal waves
    Theoretical study
  • Summary

4
Seiches in non-rotating lake
ts
h
x
h
u
L
5
Modes
1st mode (r1)
2nd mode (r2)
3rd mode (r3)
Currents
Decomposition into modes
6
Modal analysis
7
Modal analysis
Each mode evolve independently
Spatial
Forcing
Temporal
r 1, 2, 3,
8
Horizontal structure excitation of internal
wave gyres in Lake Biwa
  • Understanding relationship between horizontal
    structure of modes their excitation by winds
  • Extraction of partitioning of energy input into
    different modes from simulation results

Wind stress
1
1
Temperature
Gyres
Internal waves
density
3
2
BBL
Turbulence
Bottom stress
9
Lake Biwa
Internal waves (BITEX93)
Gyres (Jun 1994)
Counter-clockwise
Clockwise
Velocity 10 15 cm s-1
10
Modes in Lake Biwa
11
Excitation - IWs





Wind
-
-
-

NE winds
H1 K dominant
12
Excitation - IWs
-



Wind



-
NE winds
H1 K dominant
NW winds
H1, 2 4 K, H1 P comparable
Winds can preferentially excite certain modes
13
Excitation - Gyres
Wind stress curl
Positive in north
Negative in south
14
Numerical Simulation
ADCP
3D hydrodynamic model ELCOM
- Spatially variable wind
- No heat transfer / No inflows outflows
ELCOM
15
Energy Partitioning
Strong winds
Excite IWs
but damp quickly
Calm periods
Gyres dominate
16
Summary 1
  • Winds excite modes that have similar velocity
    pattern in the surface layer
  • Internal waves receive large part of energy input
    from winds, and they are damped quickly
  • Gyres dominate during the calm periods due to
    slower damping

Published as Shimizu, K., J. Imberger, M.
Kumagai. 2007. Horizontal structure and
excitation of primary motions in a strongly
stratified lake. Limnol. Oceanogr. 52 2641-2655
17
Energetics damping of internal waves in Lake
Kinneret
  • Estimate damping rates and energetics of internal
    waves from thermistor chain data
  • Illustrate effects of internal wave structure on
    near-bottom mass transport

Wind stress
1
1
Temperature
Gyres
Internal waves
density
2
3
BBL
Turbulence
Bottom stress
18
Lake Kinneret
19
Internal wave modes in Lake Kinneret
20
Mode fitting
- Fit five dominant internal waves
Optimize a0(m) Td(m)
21
Damping rates energy dissipation
Damping time Td (day)
Period T (hr)
Dissipation rate D (GJ day-1)
Internal wave
V2H3 Kelvin
2.1
1.2
23.3
V1H1 Kelvin
1.7
1.7
22.1
V2H1 Poincare
3.3
0.2
17.3
V1H3 Kelvin
0.83
0.3
10.8
V1H1 Poincare
1.1
0.4
10.0
If internal waves are damped by bottom friction,
Energy dissipation Work done against bottom
friction
Cb 0.0029
D Rate of energy dissipation
Cb Bottom drag coefficient
vb Estimated velocity field
22
Near-bottom transport
Current
r
Turbulence
Entrainment of hypolimnetic water
BBL
Resuspension / deposition
Diffusion of soluble materials
Bottom friction
Dissipation rate
Data source Marti Imberger (2006)
Hydrobiologia
Data sourceLemckert et al. (2004) J. Hydraul.
Eng.
23
Near-bottom transport
Mass transfer coefficient(BBL-sediment)
Bottom shear stress(resuspension)
Entrainment rate(hypolimnion - BBL)
Lorke et al. (2003) Limnol. Oceanogr.
Gloor et al. (2000) J. Geophys. Res.
Internal wave structure
Large spatial variability
24
Summary 2
  • Proposed a method that
  • extracts energy budgets and damping rates of
    individual internal waves from field data
  • estimates spatial variability near-bottom mass
    transport
  • 2. Internal waves were damped primarily by bottom
    friction
  • 3. Spatial structure of internal waves can cause
    large spatial variability of near-bottom
    transport processes

In press as Shimizu, K. J. Imberger.
Energetics and damping of internal waves in a
strongly stratified lake. Limnol. Oceanogr.
25
Damping mechanisms of internal waves in a
stratified rotating basin
  • Understanding how internal waves are damped by
    friction confined in thin bottom boundary layers

Wind stress
1
1
Temperature
Gyres
Internal waves
density
3
2
BBL
Turbulence
Bottom stress
26
Simplified problem
Circular basin
Flat bottom, vertical sidewall
Shallow basin (H/Rltlt1)
Linearly stratified
Rotating with frequency 2f
Viscosity is included only in thin boundary
layers
2f
Frequency (compared to f)
Low
High
r
H
Damping mechanism
Spin-down
Wave cancelling
Johns (1968)Dore (1968) Mei Liu (1973)
Barcilon Pedlosky (1967)Greenspan(1968)Walin
et al. (1969)Gill (1982)
2R
27
Internal wave cancelling
z
r
Energy flux F pressure p velocity w
28
Spin-down
2f
r
H
Ekman layer
Bottom Corner Region
2R
29
Bottom boundary layer structure
Ekman layer
t T/4
t T/4
t T/4
t T/4
t 0
t 0
t 0
t 0
w 3f
w 0.1f
w f
w 1.1f
w 0.9f
Direction of boundary layer transport
45o to the left
45o to the right
Parallel
30
Damping rates
R1A1 Kelvin
g / 2w
Internal wave cancelling
Spin-down
R1A1 Poincare
g / 2w
Burger number
31
Comparison
Circular basin
R 6.4 km
H 30 m
Antenucci Imberger (2001)
2p/f 22.4 hr
S 0.6
n 10-4 m2 s-1
Yeates Imberger (2001)
Period (hr)
Damping time (day)
Field data
Theory
5.8
1.7
22.1
V1H1 Kelvin
2.6
V1H1 Poincare
1.1
10.0
32
Summary 3
  • Thin boundary layers can cause damping of
    internal waves without diffusion through a
    combination of internal wave cancelling and
    spin-down.
  • Predicted and observed damping rates were
    comparable, but theory under-predicted damping
    rates.

Under internal review. To be submitted to J.
Fluid Mech.
33
Conclusions
  • Winds excite modes that have similar surface
    velocity structure with the wind stress pattern
  • Internal waves receive dominant part of the
    energy input from winds and provide the energy to
    near-bottom mixing
  • Gyres are damped slowly and important for
    long-term horizontal transport
  • Spatial structure of internal waves can cause
    significant variability of near-bottom mass
    transport processes
  • Internal waves are damped quickly by bottom
    friction through internal wave cancelling and
    spin-down

34
Acknowledgements
  • Jörg
  • Japanese Government Scholarship, Tokyo-Tech
    Long-term study support program CWR ad-hoc
    scholarship
  • Lake Biwa Research Institute (M. Kumagai, C.
    Jiao)
  • J. Antenucci, C. Dallimore, A. Gomez-Giraldo, T.
    Johnson, P. Okely, T. Shintani
  • Officemates P. Yeates, S. Morillo, A. de la
    Funte, C. Boon, P. Okely, P. Huang
  • Students staff in CWR SESE
  • Family
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