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Effect of directional movement on animal food search
Sarafa Iyaniwura
Institute of Applied Mathematics,University of British Columbia, Vancouver.
April 6, 2017
Sarafa Iyaniwura Math521: Numerical Analysis of PDEs April 6, 2017 1 / 13
Siniff, Donald Blair, and C. R. Jessen. ”A simulation model of animal movement
patterns.” Advances in ecological research 6 (1969): 185-219
Figure: A fox and a rabbit. Ref: Tom UlrichStone/Getty Images (left)
Question: What is the effect of directional motion on the time to get prey?
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Literature review
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Geometry of the region of animal movement
What do we want do to?
use first passage time theory to compare the search time to prey foran animal performing directional motion (biased random walk) andthat which performs a random walk (unbaised random walk)
Sarafa Iyaniwura Math521: Numerical Analysis of PDEs April 6, 2017 4 / 13
First Passage Time
Let T1 be the mean first passage time for the Red Fox to find a prey andT2 is the second moment of the first passage time distribution. Then
D∆T1 + v · ∇T1 = −1, in Ωk⋃
i=1
Ωi ,
∇T1 · n = 0 on ∂Ω, and T1 = 0 on ∂Ωi , for i = 1, 2, . . . , k.
(1)
And the second moment satisfies
D∆T2 + v · ∇T2 = −T1, in Ωk⋃
i=1
Ωi ,
∇T2 · n = 0 on ∂Ω, and T2 = 0 on ∂Ωi , for i = 1, 2, . . . , k,
(2)
where D is the diffusion coefficient of the predator, and v is its velocity.Variance:
V = T2 − T 21 . (3)
Sarafa Iyaniwura Math521: Numerical Analysis of PDEs April 6, 2017 5 / 13
Weak Formulation and Linear Finite Element
Let u ∈ V be a test function, then the weak formulation of theproblems are
D
∫W∇T1 · ∇u dx −
∫W
(v · ∇T1) u dx =
∫W
u dx
And the second moment,
D
∫W∇T2 · ∇u dx −
∫W
(v · ∇T2) u dx =
∫W
T1 u dx
where W = Ωk⋃
i=1Ωi .
this problem is solved using linear finite element method
D Kh−→T − V h−→T =−→f
where Kh and V h are the stiffness and advection matrices respectively.
Sarafa Iyaniwura Math521: Numerical Analysis of PDEs April 6, 2017 6 / 13
Numerical results
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Parameters: D = 0.41 km2/h, v = 0.085 km/h, R = 1 km, prey radius = 50cm)
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Parameters:
D = 0.41 km2/h, v = 0.085 km/h, area of region = 4 km2, prey radius = 50cm)
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Sources of error
Approximation error/interpolation error
triangulation of the domain
Quadrature Error
using numerical quadrature to evaluate integrals likeKi,j =
∫T∇φi · ∇φj dx that arise when constructing the stiffness
matrix
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Conclusion and future work
Conclusion
depending on where the animal is starting from, directional motion mayor may not favour the animal
Future work
consider a more realistic scenario where the rabbits are also moving
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Some references
Kurella, Venu, et al. ”Asymptotic analysis of first passage timeproblems inspired by ecology.” Bulletin of mathematical biology 77.1(2015): 83-125.
Siniff, Donald Blair, and C. R. Jessen. ”A simulation model of animalmovement patterns.” Advances in ecological research 6 (1969):185-219.
McKenzie, Hannah W., Mark A. Lewis, and Evelyn H. Merrill. ”Firstpassage time analysis of animal movement and insights into thefunctional response.” Bulletin of mathematical biology 71.1 (2009):107-129.
Gardiner, C. W. ”Handbook of stochastic methods for physics,chemistry and the natural sciences.” Applied Optics 25 (1986): 3145.
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