Transcript Slide 1

RIVER RESPONSE TO POST-GLACIAL SEA
LEVEL RISE: THE FLY-STRICKLAND RIVER
SYSTEM, PAPUA NEW GUINEA
Gary Parker, Tetsuji Muto, Yoshihisa
Akamatsu, Bill Dietrich, Wes Lauer
RIVER MOUTHS, LIKE NAVELS, HAVE TWO BASIC TYPES:
INNIES AND OUTIES
The delta of the Mississippi River
protrudes into the Gulf of Mexico
THE EAST COAST OF
THE UNITED STATES,
HOWEVER, IS
DOMINATED BY
DROWNED RIVER
MOUTHS
Delaware River
Susquehanna River
Potomac River
Delaware Bay
Chesapeake Bay
SO WHY THE DIFFERENCE??
Outie
Innie
SEA LEVEL HAS RISEN ABOUT 120 METERS SINCE THE
END OF THE LAST ICE AGE
Years before present
How does a river mouth respond to sea level rise?
• Does a delta continue to prograde into the ocean?
• Or does the sea drown the delta and invade the river valley (transgression)?
EXPERIMENTS OF MUTO: RISING BASE LEVEL,
SHORELINE STARVATION AND AUTORETREAT!
VIDEO CLIP
PHOTOGRAPH AND INTERPRETATION OF ONE OF THE
EXPERIMENTS OF MUTO
autoretreat
autobreak
shoreline trajectory
topset
foreset
THE ESSENTIAL RESULTS OF MUTO’S EXPERIMENTS
• When constant sea level is maintained the shoreline and
delta prograde outward (shoreline regresses).
• If sea level rises at a constant rate, the shoreline first
progrades outward, but the progradation rate is
suppressed.
• If sea level continues to rise, progradation is eventually
reversed and the shoreline is pushed landward.
• If sea level still continues to rise, sediment transport at the
shoreline drops to zero, the delta is drowned and the
shoreline rapidly moves landward (transgresses).
Whether or not a delta continues to prograde, or instead is drowned
depends on a) the rate and duration of sea level rise (higher values favor
drowning) and sediment supply at the bedrock-alluvial transition (a
higher value favors continued progradation).
MORPHODYNAMIC MODELING OF DELTA RESPONSE TO
SEA LEVEL RISE
Modeling of Muto’s highly simplified 1D laboratory deltas is a first step toward
modeling the response of 2D field river mouths to sea level rise.
THE FUN PART IS THE PRESENCE OF THREE MOVING BOUNDARIES!!!
sediment feed
topset-foreset break
(shoreline)
here!
here!
bedrock-alluvial transition
foreset-basement break
SOME SAMPLE RESULTS
14.6
0.15
eta m
0.1
0.05
0
-0.05
-0.1
-1
-0.5
0
xm
0.5
0 sec
35.9 sec
71.7 sec
107.6 sec
143.4 sec
179.2 sec
215.1 sec
250.9 sec
286.8 sec
322.7 sec
358.5 sec
394.4 sec
430.2 sec
466.1 sec
501.9 sec
537.8 sec
573.6 sec
609.5 sec
645.3 sec
681.2 sec
717 sec
APPLICATION TO LARGE, LOW-SLOPE SAND-BED RIVERS:
HOW DID THEY RESPOND TO SEA LEVEL RISE?
All such rivers flowing into the sea were subject to ~ 120 m of eustatic
sea level rise since the end of the last glaciation.
DELTA PROGRADATION
Even when the body of water in question (lake or the ocean) maintains constant
base level, progradation of a delta into standing water forces long-term
aggradation and an upward-concave profile. Both the channel and the floodplain
must prograde into the water.
Missouri River prograding
into Lake Sakakawea,
North Dakota.
Image from NASA
website:
https://zulu.ssc.nasa.gov/mrsid/mrsid.pl
Wash load cannot be neglected: it is needed to form the floodplain as
the river aggrades.
Missouri River prograding
into Lake Sakakawea,
North Dakota.
Image from NASA
website:
https://zulu.ssc.nasa.gov/mrsid/mrsid.pl
FORMULATION OF THE PROBLEM: EXNER
Sediment is carried in channel but deposited across the floodplain due to
aggradation forced by sea level rise. Adapting the formulation of Chapter 15,
where qtbf denotes the bankfull (flood) value of volume bed material load per unit
width qt, qwbf denotes the bankfull (flood) value of volume wash load per unit width
and  denotes channel sinuosity,

sB f (1   p )x v  sIf Bbf (qtbf  qwbf ) x  sIf Bbf (qtbf  qwbf ) x  x
t
x
  , Qtbf  Bbf qtbf
x v
xv
x
B
xv
(1  p )
Bf
xv+xv
, Qwbf  Bbf qwbf
Qwbf 

I  Q
  f  tbf 

t
Bf  x
x 
FORMULATION OF THE PROBLEM: EXNER contd.
It is assumed that for every one unit of bed material load deposited  units of
wash load are deposited to construct the channel/floodplain complex;
Q wbf
Q tbf

x
x
Thus the final form of Exner becomes
xv
x
B
Bf
xv+xv
xv

If (1   ) Qtbf
(1  p )
 
t
Bf
x
River channels are self-formed! For example, channel width must be
a computed rather than specified parameter.
bf 50 
Hbf S
RD50
Qbf
2
gD50 D50
ˆ 
, Q
sand  bed : bf 50  1.86
gravel  bed :
bf 50  0.0487
1.E+01
1.E+00
bf 50
1.E-01
Gravel
Gravel Average
Sand
Sand Average
1.E-02
1.E-03
1.E+02
1.E+04
1.E+06
1.E+08
ˆ
Q
1.E+10
1.E+12
1.E+14
Closure using constant Chezy resistance coefficient, set channelforming Shields number form* and Engelund-Hansen relation for total
bed material load
B
1

D Cz 2 R EH form


2.5
R
Qtbf
S
Cz EHform Qbf
H

2 Qbf
 Cz EH (  form )
D
Qtbf
EH  0.05 , nt  2.5
Qtbf
 Cz EH form 

Qbf S

R


Qtbf
gD D2
A RIVER SYSTEM AFFECTED BY RISING SEA LEVEL
The Fly-Strickland River System in
Papua New Guinea has been
profoundly influenced by Holocene
sea level rise.
Fly River
Strickland
River
Image from NASA website:
https://zulu.ssc.nasa.gov/mrsid/mrsid.pl
Fly River
SOME CALCULATIONS APPLIED TO THE FLY-STRICKLAND
RIVER SYSTEM, PAPUA NEW GUINEA
Gravel-sand transition is
approximated as bedrocksand transition.
CASE OF CONSTANT SEA LEVEL
Bed Profiles
200
180
0 yr
2000 yr
4000 yr
6000 yr
8000 yr
10000 yr
12000 yr
final w.s.
Elevation m
160
140
120
100
80
60
40
20
0
-200000
0
200000
400000
Downvalley distance m
600000
800000
CASE OF 1 MM/YEAR RISE AFTER YEAR 2000
Bed Profiles
200
180
0 yr
2000 yr
4000 yr
6000 yr
8000 yr
10000 yr
12000 yr
final w.s.
Elevation m
160
140
120
100
80
60
40
20
0
-200000
0
200000
400000
Downvalley distance m
600000
800000
CASE OF 2 MM/YEAR RISE AFTER YEAR 2000
Bed Profiles
200
180
0 yr
2000 yr
4000 yr
6000 yr
8000 yr
10000 yr
12000 yr
final w.s.
Elevation m
160
140
120
100
80
60
40
20
0
-200000
0
200000
400000
Downvalley distance m
600000
800000
CASE OF 5 MM/YEAR RISE AFTER YEAR 2000
Bed Profiles
200
180
0 yr
2000 yr
4000 yr
6000 yr
8000 yr
10000 yr
12000 yr
final w.s.
Elevation m
160
140
120
100
80
60
40
20
0
-200000
0
200000
400000
Downvalley distance m
600000
CASE OF 10 MM/YEAR RISE AFTER YEAR 2000
Bed Profiles
200
180
0 yr
2000 yr
4000 yr
6000 yr
8000 yr
10000 yr
12000 yr
final w.s.
Elevation m
160
140
120
autoretreat!!!
100
80
60
40
20
0
-200000
0
200000
400000
Downvalley distance m
600000
CASE OF 10 MM/YEAR RISE AFTER YEAR 2000
SEDIMENT SUPPLY
INCREASED BY FACTOR
450 OF 2.17
Bed Profiles
0 yr
2000 yr
4000 yr
6000 yr
8000 yr
10000 yr
12000 yr
final w.s.
400
Elevation m
350
300
250
200
150
100
50
0
-20000 -10000
0
0
0
100000 200000 300000 400000 500000 600000 700000
Downvalley distance m
Recovery from autoretreat?
CONCLUSIONS
Morphodynamics is fun.
Autoretreat can be
successfully reproduced in
a moving-boundary
morphodynamic model.