The benefit of this approximation is that is converted from an exponent to a multiplicative factor. This can greatly simplify mathematical expressions (as in the example below) and is a common tool in physics.
The approximation can be proven several ways, and is closely related to the binomial theorem. By Bernoulli's inequality, the left-hand side of the approximation is greater than or equal to the right-hand side whenever and .
where and may be real or complex can be expressed as a Taylor Series about the point zero.
If and ≪ , then the terms in the series become progressively smaller and it can be truncated to
.
This result from the binomial approximation can always be improved by
keeping additional terms from the Taylor Series above. This is
especially important when starts to approach one, or when evaluating a more complex expression where the first two terms in the Taylor Series cancel (see example).
Sometimes it is wrongly claimed that ≪ is a sufficient condition for the binomial approximation. A simple counterexample is to let and . In this case but the binomial approximation yields . For small but large , a better approximation is:
Examples
Example simplification
Consider the following expression where and are real but ≫ .
The mathematical form for the binomial approximation can be recovered by factoring out the large term and recalling that a square root is the same as a power of one half.
Evidently the expression is linear in when ≫ which is otherwise not obvious from the original expression.
Example keeping the quadratic term
Consider the expression:
where and ≪ . If only the linear term from the binomial approximation is kept then the expression unhelpfully simplifies to zero
.
While the expression is small, it is not exactly zero. It is
possible to extract a nonzero approximate solution by keeping the
quadratic term in the Taylor Series, i.e. so now,
This result is quadratic in which is why it did not appear when only the linear in terms in were kept.