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Introduction to the Modeling and Analysis of Complex Systems

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13.2. FUNDAMENTALS OF VECTOR CALCULUS 229finally facing systems with infinitely many variables!But <strong>of</strong> course, we are not actually capable <strong>of</strong> modeling or analyzing systems made <strong>of</strong>infinitely many variables. In order <strong>to</strong> bring <strong>the</strong>se o<strong>the</strong>rwise infinitely complex ma<strong>the</strong>maticalmodels down <strong>to</strong> something manageable for us who have finite intelligence <strong>and</strong> lifespan,we usually assume <strong>the</strong> smoothness <strong>of</strong> function f. This is why we can describe <strong>the</strong> shape<strong>and</strong> behavior <strong>of</strong> <strong>the</strong> function using well-defined derivatives, which may still allow us <strong>to</strong>study <strong>the</strong>ir properties using analytical means 1 .13.2 Fundamentals <strong>of</strong> Vec<strong>to</strong>r CalculusIn order <strong>to</strong> develop continuous field models, you need <strong>to</strong> know some basic ma<strong>the</strong>maticalconcepts developed <strong>and</strong> used in vec<strong>to</strong>r calculus. A minimalistic quick review <strong>of</strong> thoseconcepts is given in <strong>the</strong> following.Con<strong>to</strong>urA con<strong>to</strong>ur is a set <strong>of</strong> spatial positions x that satisfyf(x) = C (13.2)for a scalar field f, where C is a constant (see an example in Fig. 13.2). Con<strong>to</strong>ursare also called level curves or surfaces.GradientA gradient <strong>of</strong> a scalar field f is a vec<strong>to</strong>r locally defined as⎛ ⎞∂f∂x 1∂f∇f =∂x 2. (13.3)⎜ .⎟⎝ ∂f ⎠∂x n1 But we should also be aware that not all physically important, interesting systems can be represented bysmooth spatial functions. For example, electromagnetic <strong>and</strong> gravitational fields can have singularities wheresmoothness is broken <strong>and</strong> state values <strong>and</strong>/or <strong>the</strong>ir derivatives diverge <strong>to</strong> infinity. While such singularitiesdo play an important role in nature, here we limit ourselves <strong>to</strong> continuous, smooth spatial functions only.

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