Planktonic Population in a Spatially Variable Environment Yue-Kin - - PowerPoint PPT Presentation
Planktonic Population in a Spatially Variable Environment Yue-Kin - - PowerPoint PPT Presentation
Planktonic Population in a Spatially Variable Environment Yue-Kin Tsang Courant Institute of Mathematical Sciences New York University Daniel Birch and William R. Young Scripps Institution of Oceanography, UCSD What is Plankton? tiny
What is Plankton?
tiny open-water bacteria, plants or animals that have limited or no swimming ability transported through the water by currents and tides
Phytoplankton Macrozooplankton Zooplankton
One gallon of water from the Chesapeake Bay can contain more than 500,000 zooplankton and
- ne
drop may contain thousands of individual phytoplankton!!
Why Study Plankton Population?
carbon fixation: CO2 concentration in atmosphere would be doubled without plankton indicators of nutrient level and other water quality conditions base
- f
the food chain that support commercial fisheries plankton blooms that deplete oxygen
Population Model
∂P ∂t + u · ∇P = γP − ηP 2 + κ∇2P
advection small-scale diffusion growth saturation
✁ ✁ ✕ ✂ ✂✂ ✍ ❈ ❈ ❈ ❖ ❅ ❅ ■
Population Model
∂P ∂t + u · ∇P = γP − ηP 2 + κ∇2P
advection small-scale diffusion growth saturation
✁ ✁ ✕ ✂ ✂✂ ✍ ❈ ❈ ❈ ❖ ❅ ❅ ■
2D Lagrangian Chaotic Flow (U, k, τ)
- u(
x, t)= √ 2U cos[ky + α(t)]ˆ i , nτ ≤ t < (n+ 1
2)τ
√ 2U cos[kx + β(t)] ˆ j , (n+ 1
2)τ ≤ t < (n+1)τ
Spatially uniform γ and η: P → η/γ
Population Model
∂P ∂t + u · ∇P = γ( x)P − ηP 2 + κ∇2P
advection small-scale diffusion growth saturation
✁ ✁ ✕ ✂ ✂✂ ✍ ✄ ✄✄ ✗ ❇ ❇ ▼
2D Lagrangian Chaotic Flow (U, k, τ)
- u(
x, t)= √ 2U cos[ky + α(t)]ˆ i , nτ ≤ t < (n+ 1
2)τ
√ 2U cos[kx + β(t)] ˆ j , (n+ 1
2)τ ≤ t < (n+1)τ
Spatially uniform γ and η: P → η/γ Environmental variability : γ = γ(
x)
Oasis and Desert
interested in the situation where γ(
x) > 0 in some
region (oasis) and γ(
x) ≤ 0 in the complementary
region (desert)
γ ≤ 0 γ > 0
two cases: (1) γ > 0 and (2) γ < 0
An Example
doubly periodic domain domain size : 2π × 2π grid : 1024 × 1024
γ( x) = 0.2 + 0.8 cos x η = 1.0 κ ∼ 10−4 U = π k = 1 τ = 1/4
π 2π x
- 0.6
0.0 1.0 γ(x)
Biomass and Productivity
Biomass
B = P = lim
T→∞
1 TAΩ T dt
- Ω
d x P( x, t)
Productivity
P = γP
For the above example: B ≈ 0.24 and P ≈ 0.14 (note γ = 0.2)
Biomass and Productivity
Biomass
B = P = lim
T→∞
1 TAΩ T dt
- Ω
d x P( x, t)
Productivity
P = γP
For the above example: B ≈ 0.24 and P ≈ 0.14 (note γ = 0.2) We shall obtain bounds on B and P in terms of γ and η
Bounds on B and P
∂P ∂t + u · ∇P = γP − ηP 2 + κ∇2P (∗) (∗)
- γP − ηP 2
= 0 B = P + m
- γP − ηP 2
(m > 0) = m 4η
- γ + 1
m 2 − mη
- (P − #)2
Bounds on B and P
∂P ∂t + u · ∇P = γP − ηP 2 + κ∇2P (∗) (∗)
- γP − ηP 2
= 0 B = P + m
- γP − ηP 2
(m > 0) ≤ m 4η
- γ + 1
m 2 −mη
- (P − #)2
minimizing RHS with respect to m gives upper bound for B,
B ≤
- γ2 + γ
2η
Bounds on B and P
(∗)/P γ − η P + κ
- |∇ ln P|2
= 0 γ η ≤ B ≤
- γ2 + γ
2η
Bounds on B and P
(∗)/P γ − η P + κ
- |∇ ln P|2
= 0 γ η ≤ B ≤
- γ2 + γ
2η
Cauchy-Schwarz Inequality: AB ≤
- A2 B2,
η P2 ≤ η
- P 2
= γP ≤
- γ2 P 2
γ2 η ≤ P ≤
- γ2
η
Bounds on B and P
For our example with γ(
x) = 0.2 + 0.8 cos x and η = 1,
0.15 0.20 0.25 0.30 0.35 0.40 0.45 0.0 0.1 0.2 0.3 0.4
P B
Simultaneous Bounds
P = γP + α[B − P] + β[γP − η
- P 2
]
0.15 0.20 0.25 0.30 0.35 0.40 0.45 0.0 0.1 0.2 0.3 0.4
f1(B) ≤ P ≤ f2(B) P B
What happen when γ < 0?
Recall γ
η ≤ B ≤
√
γ2+γ 2η
γ > 0 implies population will never become extinct
What happen when γ < 0?
Recall γ
η ≤ B ≤
√
γ2+γ 2η
γ > 0 implies population will never become extinct
When γ < 0, extinction (B = 0) is a possibility
π 2π
x
- 0.5
0.0 1.0
γ(x)
Survival-Extinction Transition
2.4 2.6 2.8 3.0 3.2 3.4 3.6 3.8
U
0.00 0.02 0.04 0.06
<P>
transition occurs at U = Uc ≈ 3.52, prediction for Uc?
Eddy (Effective) Diffusivity
Characterize spreading using X2: a pure diffusive process
∂φ ∂t = κ∇2φ ⇒ X2 = 4κt
pure advection by our flow model
∂φ ∂t + u · ∇φ = 0 ⇒ X2 = U 2τ 2 t
may parameterize the effect of
u on large-scale φ by D, ∂φ ∂t = D∇2φ
with
D = U 2τ 8
Theory for Uc
∂P ∂t + u · ∇P = γP − ηP 2 + κ∇2P
consider small κ near transition: ηP 2 ≈ 0 parameterization using eddy diffusivity D
∂P ∂t = γP + D∇2P
Linear stability analysis about P = 0: P = est ˆ
P
maximum s = 0 ⇒ extinction, thus critical Dc given by
∇2P + γ Dc P = 0
and
Dc = U 2
c T
8
Theory vs. Simulation
- 1.0
- 0.8
- 0.6
- 0.4
- 0.2