Planktonic Population in a Spatially Variable Environment Yue-Kin - - PowerPoint PPT Presentation

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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


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SLIDE 1

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

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SLIDE 2

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!!

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SLIDE 3

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

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SLIDE 4

Population Model

∂P ∂t + u · ∇P = γP − ηP 2 + κ∇2P

advection small-scale diffusion growth saturation

✁ ✁ ✕ ✂ ✂✂ ✍ ❈ ❈ ❈ ❖ ❅ ❅ ■

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SLIDE 5

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

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SLIDE 6

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)

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SLIDE 7

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

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SLIDE 8

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)

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SLIDE 9

Biomass and Productivity

Biomass

B = P = lim

T→∞

1 TAΩ T dt

d x P( x, t)

Productivity

P = γP

For the above example: B ≈ 0.24 and P ≈ 0.14 (note γ = 0.2)

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SLIDE 10

Biomass and Productivity

Biomass

B = P = lim

T→∞

1 TAΩ T dt

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

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SLIDE 11

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
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SLIDE 12

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

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SLIDE 13

Bounds on B and P

(∗)/P γ − η P + κ

  • |∇ ln P|2

= 0 γ η ≤ B ≤

  • γ2 + γ

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SLIDE 14

Bounds on B and P

(∗)/P γ − η P + κ

  • |∇ ln P|2

= 0 γ η ≤ B ≤

  • γ2 + γ

Cauchy-Schwarz Inequality: AB ≤

  • A2 B2,

η P2 ≤ η

  • P 2

= γP ≤

  • γ2 P 2

γ2 η ≤ P ≤

  • γ2

η

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SLIDE 15

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

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SLIDE 16

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

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SLIDE 17

What happen when γ < 0?

Recall γ

η ≤ B ≤

γ2+γ 2η

γ > 0 implies population will never become extinct

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SLIDE 18

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)

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SLIDE 19

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?

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SLIDE 20

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

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SLIDE 21

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

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SLIDE 22

Theory vs. Simulation

  • 1.0
  • 0.8
  • 0.6
  • 0.4
  • 0.2

0.0

< γ >

2 3 4 5 6 7 8

Uc

theory simulation

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SLIDE 23

Summary

we study plankton population using an advection-diffusion logistic-growth model in a domain divided into oasis (γ > 0) and desert (γ < 0) for γ > 0, population never extinct and we obtain bounds on the biomass and productivity for γ < 0, population becomes extinct when the velocity is large, we make prediction to such critical velocity Uc