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7/29/2019 Lec02 Review of Equations
1/20
Review of conservation equations
State, Mass and Momentum
7/29/2019 Lec02 Review of Equations
2/20
Equation of State (EOS-80)
Determines water density from T, S, and P
),,(/1),,(/1)0,,(),,( PTSPTSKPTSPTS 22/3)0,,(/1)0,,( DSCSBSATSTS
22/32/3 )()(),,( PNSMPJSISHGSFSEPTSK A through Nare polynomials
Tis temperature in oC
S salinity
Ppressure in bars
Ksecant bulk modulus measure of compresibility
7/29/2019 Lec02 Review of Equations
3/20
A B C D
T0 999.842594 8.24493E-1 -5.72466E-3 4.8314E-4
T1 6.793952E-2 -4.0899E-3 1.0227E-4
T2 -9.095290E-3 7.6438E-5 -1.6546E-6
T3 1.001685E-4 -8.2467E-7
T4 -1.120083E-6 5.3875E-9
T5 6.536332E-9
E F G
T0 19652.21 54.6746 7.944E-2
T1 148.4206 -0.603459 1.6483E-2
T2 -2.327105 1.09987E-2 -5.3009E-4
T3 1.360477E-2 -6.1670E-5
T4 -5.155288E-5
H I J
T0 3.239908 2.2838E-3 1.91075E-4
T1 1.43713E-3 -1.0981E-5
T2 1.16092E-4 -1.6078E-6
T3 -5.77905E-7
M N
T0 8.50935E-5 -9.9348E-7
T1 -6.12293E-6 2.0816E-8
T2 5.2787E-8 9.1697E-10
Check values:
489.1069)1000,5,35(
343.1023)0,25,35(
1000
7/29/2019 Lec02 Review of Equations
4/20
Greater influence of salinity on density
90 % of Ocean Water
Mean T & S for
World Ocean
7/29/2019 Lec02 Review of Equations
5/20
Effects of Temperature and Salinity on Density
T
1
S
1
Thermal Expansion Saline Contraction
x 10-4 oC-1 x 10-4 S-1
Density changes by 0.2 kg/m3 for a T change of 1oC,
and by 0.8 kg/m3 for a S change of 1.
7/29/2019 Lec02 Review of Equations
6/20
x
z
y
dy
dz
dx
Flux of mass in (kg/s) = dzdyu Flux of mass out (kg/s) = dzdyu dzdydxu
x
Net Flux of mass in
x = dzdydxux
Net Flux of mass in y = dzdydxvy
Net Flux of mass in z = dzdydxwz
dxux
u
, u
, w
, v
u
Mass per area per time
(kg/(m2 s))
7/29/2019 Lec02 Review of Equations
7/20
The change of mass per unit time going through the volume element is:
And the change of mass per unit time per unit volume is:
dzdydxtt
M
dzdydxw
zv
yu
xdzdydx
t
0 wzvyuxt which is the same as:
0
z
w
y
v
x
u
zwyvxut
01
z
w
y
v
x
u
Dt
D
or
7/29/2019 Lec02 Review of Equations
8/20
This is the Continuity Equation or Equation ofConservation of Mass
How valid is the Boussinesq approximation in the OCEAN?
How would you determine that?
1 sigma-t throughout one day = 1 / (24*3600.) = 1.1510-5
01
z
w
y
v
x
u
Dt
D
0
Dt
DTaking
Boussinesq approximation
0 zw
y
v
x
u
x
u]O[10
km100
m/s0.1 6-
Dt
D
810O1 Dt
DBut
7/29/2019 Lec02 Review of Equations
9/20
Continuity Equation in Bulk Form: b0 VEVPR
z
x
7/29/2019 Lec02 Review of Equations
10/20
Conservation of Salt:
ydiffusivitDt
DS
z
S
zK
zy
S
yK
yx
S
xK
xz
Sw
y
Sv
x
Su
t
S
Conservation of Heat:
z
T
zzy
T
yyx
T
xxz
Tw
y
Tv
x
Tu
t
T
Equation of State:
SpTS 11000],,[
7/29/2019 Lec02 Review of Equations
11/20
Continuity Equation in Bulk Form: b0 VEVPR
Sb
S0
Salt Conservation Equation in Bulk Form: VbSb =V0S0
z
x
7/29/2019 Lec02 Review of Equations
12/20
Conservation of Momentum (Equations of Motion)
Fam
m
Fa
z
ww
y
wv
x
wu
t
w
z
vw
y
vv
x
vu
t
vz
uw
y
uv
x
uu
t
u
dt
Vda
7/29/2019 Lec02 Review of Equations
13/20
mF Pressure gradient + friction + tides + gravity+ CoriolisPressure gradient: Barotropic and Baroclinic
Friction: Surface, bottom, internal
Tides: Boundary condition
Gravity: Only in the vertical
Coriolis: Only in the horizontal
REMEMBER, these are FORCES PER UNIT MASS
7/29/2019 Lec02 Review of Equations
14/20
mF Pressure gradient + friction + tides + gravity+ CoriolisPressure gradient: Barotropic and Baroclinic
Friction: Surface, bottom, internal
Tides: Boundary condition
Gravity: Only in the vertical
Coriolis: Only in the horizontal
REMEMBER, these are FORCES PER UNIT MASS
7/29/2019 Lec02 Review of Equations
15/20
z
h dzgPHydrostatic Pressure
Pressure gradient force per unit mass
x
P
1
dzgPPz
a Total Pressure
dzxgxgxP za
1
Note that even if the density is constant with depth, the horizontal pressure gradient
increases with depth if there is a horizontal density gradient
Barometric Barotropic Baroclinic
7/29/2019 Lec02 Review of Equations
16/20
mF Pressure gradient + friction + tides + gravity+ CoriolisPressure gradient: Barotropic and Baroclinic
Friction: Surface, bottom, internal
Tides: Boundary condition
Gravity: Only in the vertical
Coriolis: Only in the horizontal
REMEMBER, these are FORCES PER UNIT MASS
7/29/2019 Lec02 Review of Equations
17/20
Friction
z
uA
zy
uA
yx
uA
xzyx
@ surface:
WWC
z
uA
xdas
z
@ bottom: VCrruVuCVuC
z
uA
bb
bb
z
;
@ interior: 22
;?
z
v
z
u
z
g
RiRifzuA
z
7/29/2019 Lec02 Review of Equations
18/20
mF Pressure gradient + friction + tides + gravity+ CoriolisPressure gradient: Barotropic and Baroclinic
Friction: Surface, bottom, internal
Tides: Boundary condition
Gravity: Only in the vertical
Coriolis: Only in the horizontal
REMEMBER, these are FORCES PER UNIT MASS
7/29/2019 Lec02 Review of Equations
19/20
Gravity
[0, 0, g] = [0, 0, 9.81]
Coriolis
[-fv, fu, 0]
h
f
24
2sin2
7/29/2019 Lec02 Review of Equations
20/20
Fam
gz
P
z
vA
zy
vA
yx
vA
xdz
y
g
ygfu
z
vw
y
vv
x
vu
t
v
z
uA
zy
uA
yx
uA
xdz
x
g
xgfv
z
uw
y
uv
x
uu
t
u
z
zyx
z
zyx
10
0
z
w
y
v
x
u
z
S
z
K
zy
S
y
K
yx
S
x
K
xz
Sw
y
Sv
x
Su
t
S
z
T
zzy
T
yyx
T
xxz
Tw
y
Tv
x
Tu
t
T
SSpTS t 1000;11000],,[