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nr. 477 - 2011 - Institut for Natur, Systemer og Modeller (NSM)

nr. 477 - 2011 - Institut for Natur, Systemer og Modeller (NSM)

nr. 477 - 2011 - Institut for Natur, Systemer og Modeller (NSM)

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A Mathematical Appendices<br />

This appendix is dedicated to rigoristic statements of the important theorems that<br />

have been casually stated in different sections of the thesis. Other important concepts<br />

that pertain to mathematics will also be dealt with in the following sections; e.g. the<br />

Newton-Raphson method.<br />

A.1 Existence and Uniqueness Theorem<br />

A very important thing to determine when working with (systems of) differential equations,<br />

is wether the solution is unique, and in what interval the solution exist. I.e.<br />

given a set of initial conditions on the DuCa model (equations 5.6-5.10), we would like<br />

to know if the solution is unique, and if it exists <strong>for</strong> all time, t. To determine this we<br />

first need to introduce the property of Lipschitz continuity<br />

Definition 1<br />

Given a function g(x), g : R n → R n , and a domain U ⊂ R n , suppose that<br />

g(x1) − g(x2) ≤ Lx1 − x2 (A.1)<br />

where x1, x2 ∈ U, and L is the Lipschitz constant. Then we say that g is Lipschitz<br />

When g fulfills this condition we say that g is Lipschitz continuous, or that it is continuously<br />

Lipschitz.<br />

Now <strong>for</strong> the existence and uniqueness theorem itself<br />

Theorem A.1<br />

Suppose that g is Lipschitz continuous. Given an initial point x0 ∈ U, the autonomous<br />

differential equation<br />

˙x = g(x) (A.2)<br />

has a unique solution, φt(x0), that is defined on the maximal interval of existence.<br />

Basically as long as g ∈ C 1 (U), where U is a compact set, we need not be concerned<br />

about pathol<strong>og</strong>ical behavior of the solution (Lynch, 2004, p.176). Loosely put the C 1<br />

condition guarantees that pathol<strong>og</strong>ical behavior will not occur.<br />

One thing that may concern the reader is the fact that we need the differential equation<br />

to be autonomous, i.e. not explicitly dependent on time, which the DuCa model is not;<br />

cf. equation 5.8. The apoptotic wave depends explicitly on time, but we can remedy<br />

this by introducing another dimension, and an additional equation, into the system of<br />

equations, by setting t equal to, say, X. By this little trick we have made the DuCa<br />

model autonomous. In our case we have not been able to provide a analytic expression of<br />

131

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