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The simplest example is, when considering a function f(n), there is a need to describe its properties when n becomes very large. Thus, if f(n) = n2+3n, the term 3n becomes insignificant compared to n2 when n is very large. The function "f(n) is said to be asymptotically equivalent to n2 as n → ∞", and this is written symbolically as f(n) ~ n2.
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Formally, given functions f and g of a natural number variable n, one defines a binary relation
if and only if (according to Erdelyi, 1956)
This relation is an equivalence relation on the set of functions of n. The equivalence class of f informally consists of all functions g which are approximately equal to f in a relative sense, in the limit.
An asymptotic expansion of a function f(x) is in practice an expression of that function in terms of a series, the partial sums of which do not necessarily converge, but such that taking any initial partial sum provides an asymptotic formula for f. The idea is that successive terms provide a more and more accurate description of the order of growth of f. An example is Stirling's approximation.
In symbols, it means we have
for each fixed k, while some limit is taken, usually with the requirement that gk+1 = o(gk), which means the (gk) form an asymptotic scale. The requirement that the successive sums improve the approximation may then be expressed as
In case the asymptotic expansion does not converge, for any particular value of the argument there will be a particular partial sum which provides the best approximation and adding additional terms will decrease the accuracy. However, this optimal partial sum will usually have more terms as the argument approaches the limit value.
Asymptotic expansions typically arise in the approximation of certain integrals (Laplace's method, saddle-point method, method of steepest descent) or in the approximation of probability distributions (Edgeworth series). The famous Feynman graphs in quantum field theory are another example of asymptotic expansions which often do not converge.
Asymptotic analysis is a key tool for exploring the ordinary and partial differential equations which arise in the mathematical modelling of real-world phenomena. An illustrative example is the derivation of the boundary layer equations from the full Navier-Stokes equations governing fluid flow. In many cases, the asymptotic expansion is in power of a small parameter, : in the boundary layer case, this is the nondimensional ratio of the boundary layer thickness to a typical lengthscale of the problem. Indeed, applications of asymptotic analysis in mathematical modelling often centre around a nondimensional parameter which has been shown, or assumed, to be small through a consideration of the scales of the problem at hand.
The method of dominant balance is used to determine the asymptotic behavior of solutions to an ODE without solving it. The process is iterative in that the result obtained by performing the method once can be used as input when the method is repeated, to obtain as many terms in the asymptotic expansion as desired.
The process is as follows:
1. Assume that the asymptotic behavior has the form
2. Make a clever guess as to which terms in the ODE may be negligible in the limit we are interested in.
3. Drop those terms and solve the resulting ODE.
4. Check that the solution is consistent with step 2. If this is the case, then we have the controlling factor of the asymptotic behavior. Otherwise, we need to try dropping different terms in step 2.
5. Repeat the process using our result as the first term of the solution.
This differential equation cannot be solved exactly. However, it may be useful to know how the solutions behave for large x.
We start by assuming as . We do this with the benefit of hindsight, to make things quicker. Since we only care about the behavior of y in the large x limit, we set y equal to , and re-express the ODE in terms of S(x):
Now let us suppose that a solution to this new ODE satisfies
We get the dominant asymptotic behaviour by setting
If satisfies the above asymptotic conditions, then everything is consistent. The terms we dropped will indeed have been negligible with respect to the ones we kept. is not a solution to the ODE for S, but it represents the dominant asymptotic behaviour, which is what we are interested in. Let us check that this choice for is consistent:
Everything is indeed consistent. Thus we find the dominant asymptotic behaviour of a solution to our ODE:
By convention, the asymptotic series is written as:
so to get at least the first term of this series we have to do another step to see if there is a power of x out the front.
We proceed by making an ansatz that we can write
and then attempt to find asymptotic solutions for C(x). Substituting into the ODE for S(x) we find
Repeating the same process as before, we keep C' and (c-a)/x and find that
The leading asymptotic behaviour is therefore