標題: 沉浸邊界法在囊泡問題之數值模擬
Immersed Boundary Methods for Simulating Vesicle Dynamics
作者: 胡偉帆
Hu, Wei-Fan
賴明治
Lai, Ming-Chih
應用數學系所
關鍵字: 沉浸邊界法;囊泡;纳维-斯托克斯方程;immersed boundary method;vesicle;Navier-Stokes equations
公開日期: 2013
摘要: 過去數十年來,囊泡問題的動態數值問題一直是個熱門的議題。在本論文中,我們透過沉浸邊界法 (immersed boundary method)來描述囊泡的流體數學模型,公式,包含Eulerian座標系下的流體方程式以及建立在Lagrangian座標系中有關界面的變數,而這兩個座標系之間各個變數的轉換,則是藉由 Dirac delta function 來連結。本論文致力於發展簡易且精確的數值方法來模擬此流體界面問題。

首先,我們提出了一個fractional step immersed boundary method用於模擬不可延展界面之問題(不考慮bending effect)。我們證明了作用在表面張力spreading operator是surface divergence operator的斜自伴算子 (skew-adjoint)。利用這個特性,對於流體變數之離散我們可獲得一個對稱矩陣,並可使用fractional step方法解決此線性系統。我們比較了此數值方法的精確度,以及利用本方法研讀不可延展界面在shear flow底下之數值模擬。

再來我們研發出一種unconditionally stable immersed boundary method作為二維的囊泡在Navier-Stokes流體之模擬。我們用一種半隱示 (semi-implicit)的方法來表示囊泡之界面力,而與介面力相關的stretching factor則可透過其他的方程式獲得。我們證明出在本方法中,流體系統的總能量將隨時間而遞減。另外,利用projection method,對於流場我們推導出一個對稱正定的線性系統,此矩陣可利用多重網格法 (multi-grid method)有效率地計算其解。在數值實驗中,我們驗證本方法之精準度,並在效率上遠勝於傳統之顯示邊界力處裡方法。同樣我們也利用本方法研讀囊泡在二維座標底下之型變動態系統。

最後,我們延伸至三維軸對稱的囊泡問題。與其將表面張力作為一Lagrange's multiplier來迫使囊泡之不可延展性,我們定義一種spring-like表面張力作為本模型之逼近。囊泡的邊界可利用Fourier spectral來表示,並且我們可精準地計算出界面上的平均曲率、高斯曲率等等。透過一系列之數值模擬,我們展示出本方法之應用性與可靠性。我們使用本方法研讀囊泡在靜止流、重力場影響及Poiseuille flow下之動態型變問題。
Numerical simulation of vesicle dynamics has been a popular issue
for many decades. In this dissertation, a mathematical formulation
for suspension of vesicle in fluid is modeled by immersed boundary
method, where a mixture of Eulerian fluid variables and curve-linear
Lagrangian interfacial variables are used, and the linkage between
these two variables is a smoothed Dirac delta function. The purpose
of this dissertation is to develop accurate and efficient numerical
schemes for simulating vesicle dynamics through immersed boundary
method.

Firstly, we propose a fractional step immersed boundary method to
mimic dynamical system of an inextensible interface (vesicle without
bending effect). In addition to solving for the fluid variables such
as the velocity and pressure, the present problem involves finding
an extra unknown elastic tension such that the surface divergence of
the velocity is zero along the interface. By taking advantage of
skew-adjoint property between force spreading operator and surface
divergence operator, the resultant linear system of equations is
symmetric and can be solved by fractional steps so that only fast
Poisson solvers are involved. The convergent tests for present fluid
solver is performed and confirm the desired accuracy. The
tank-treading motion for an inextensible interface under a simple
shear flow has been studied extensively, and the results are in good
agreement with those obtained in literature. This part of work has
been published in SIAM Journal of Scientific Computing as in
[37].

Secondly, we develop an unconditionally stable immersed boundary
method to simulate 2D vesicle under a Navier-Stokes flow. We adopt a
semi-implicit boundary forcing approach, where the stretching factor
used in the forcing term can be computed from the derived
evolutional equation. By using the projection method to solve the
fluid equations, the pressure is decoupled and we have a symmetric
positive definite system that can be solved efficiently. The method
can be shown to be unconditionally stable, in the sense that the
total energy of fluid system is decreasing. A resulting modification
benefits from this improved numerical stability, as the time step
size can be significantly increased. The numerical result shows the
severe time step restriction in an explicit boundary forcing scheme
is avoided by present method. The part of work has been published in
East Asian Journal of Applied Mathematics as in [22].

Lastly, we extend to simulate three-dimensional axisymmetric vesicle
suspended in a Navier-Stokes flow. Instead of introducing a
Lagrange's multiplier to enforce the vesicle inextensibility
constraint, we modify the model by adopting a spring-like tension to
make the vesicle boundary nearly inextensible so that solving for
the unknown tension can be avoided. We also derive a new elastic
force from the modified vesicle energy and obtain exactly the same
form as the originally unmodified one. In order to represent the
vesicle boundary, we use Fourier spectral approximation so we can
compute the geometrical quantities on the interface more accurately.
A series of numerical tests on the present schemes have been
conducted to illustrate the applicability and reliability of the
method. We perform the convergence check for fluid variables for
present schemes. Then we study the vesicle dynamics in quiescent
flow, Poiseuille and under influence of gravity in detail. The
numerical results are shown to be in good agreement with those
obtained in literature. The part of work has been published in
Journal of Computational Physics as in [23].
URI: http://140.113.39.130/cdrfb3/record/nctu/#GT079822803
http://hdl.handle.net/11536/74675
顯示於類別:畢業論文


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