Binomial approximation
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The binomial approximation is useful for approximately calculating powers of sums of 1 and a small number x. It states that
- {\displaystyle (1+x)^{\alpha }\approx 1+\alpha x.}
It is valid when {\displaystyle |x|<1} and {\displaystyle |\alpha x|\ll 1} where {\displaystyle x} and {\displaystyle \alpha } may be real or complex numbers.
The benefit of this approximation is that {\displaystyle \alpha } 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.[1]
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 {\displaystyle x>-1} and {\displaystyle \alpha \geq 1}.
Derivations
[edit ]Using linear approximation
[edit ]The function
- {\displaystyle f(x)=(1+x)^{\alpha }}
is a smooth function for x near 0. Thus, standard linear approximation tools from calculus apply: one has
- {\displaystyle f'(x)=\alpha (1+x)^{\alpha -1}}
and so
- {\displaystyle f'(0)=\alpha .}
Thus
- {\displaystyle f(x)\approx f(0)+f'(0)(x-0)=1+\alpha x.}
By Taylor's theorem, the error in this approximation is equal to {\textstyle {\frac {\alpha (\alpha -1)x^{2}}{2}}\cdot (1+\zeta )^{\alpha -2}} for some value of {\displaystyle \zeta } that lies between 0 and x. For example, if {\displaystyle x<0} and {\displaystyle \alpha \geq 2}, the error is at most {\textstyle {\frac {\alpha (\alpha -1)x^{2}}{2}}}. In little o notation, one can say that the error is {\displaystyle o(|x|)}, meaning that {\textstyle \lim _{x\to 0}{\frac {\textrm {error}}{|x|}}=0}.
Using Taylor series
[edit ]The function
- {\displaystyle f(x)=(1+x)^{\alpha }}
where {\displaystyle x} and {\displaystyle \alpha } may be real or complex can be expressed as a Taylor series about the point zero.
- {\displaystyle {\begin{aligned}f(x)&=\sum _{n=0}^{\infty }{\frac {f^{(n)}(0)}{n!}}x^{n}\\f(x)&=f(0)+f'(0)x+{\frac {1}{2}}f''(0)x^{2}+{\frac {1}{6}}f'''(0)x^{3}+{\frac {1}{24}}f^{(4)}(0)x^{4}+\cdots \\(1+x)^{\alpha }&=1+\alpha x+{\frac {1}{2}}\alpha (\alpha -1)x^{2}+{\frac {1}{6}}\alpha (\alpha -1)(\alpha -2)x^{3}+{\frac {1}{24}}\alpha (\alpha -1)(\alpha -2)(\alpha -3)x^{4}+\cdots \end{aligned}}}
If {\displaystyle |x|<1} and {\displaystyle |\alpha x|\ll 1}, then the terms in the series become progressively smaller and it can be truncated to
- {\displaystyle (1+x)^{\alpha }\approx 1+\alpha x.}
This result from the binomial approximation can always be improved by keeping additional terms from the Taylor series above. This is especially important when {\displaystyle |\alpha x|} 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 {\displaystyle |x|\ll 1} is a sufficient condition for the binomial approximation. A simple counterexample is to let {\displaystyle x=10^{-6}} and {\displaystyle \alpha =10^{7}}. In this case {\displaystyle (1+x)^{\alpha }>22,000} but the binomial approximation yields {\displaystyle 1+\alpha x=11}. For small {\displaystyle |x|} but large {\displaystyle |\alpha x|}, a better approximation is:
- {\displaystyle (1+x)^{\alpha }\approx e^{\alpha x}.}
Example
[edit ]The binomial approximation for the square root, {\displaystyle {\sqrt {1+x}}\approx 1+x/2}, can be applied for the following expression,
- {\displaystyle {\frac {1}{\sqrt {a+b}}}-{\frac {1}{\sqrt {a-b}}}}
where {\displaystyle a} and {\displaystyle b} are real but {\displaystyle a\gg b}.
The mathematical form for the binomial approximation can be recovered by factoring out the large term {\displaystyle a} and recalling that a square root is the same as a power of one half.
- {\displaystyle {\begin{aligned}{\frac {1}{\sqrt {a+b}}}-{\frac {1}{\sqrt {a-b}}}&={\frac {1}{\sqrt {a}}}\left(\left(1+{\frac {b}{a}}\right)^{-1/2}-\left(1-{\frac {b}{a}}\right)^{-1/2}\right)\\&\approx {\frac {1}{\sqrt {a}}}\left(\left(1+\left(-{\frac {1}{2}}\right){\frac {b}{a}}\right)-\left(1-\left(-{\frac {1}{2}}\right){\frac {b}{a}}\right)\right)\\&\approx {\frac {1}{\sqrt {a}}}\left(1-{\frac {b}{2a}}-1-{\frac {b}{2a}}\right)\\&\approx -{\frac {b}{a{\sqrt {a}}}}\end{aligned}}}
Evidently the expression is linear in {\displaystyle b} when {\displaystyle a\gg b} which is otherwise not obvious from the original expression.
Generalization
[edit ]While the binomial approximation is linear, it can be generalized to keep the quadratic term in the Taylor series:
- {\displaystyle (1+x)^{\alpha }\approx 1+\alpha x+(\alpha /2)(\alpha -1)x^{2}}
Applied to the square root, it results in:
- {\displaystyle {\sqrt {1+x}}\approx 1+x/2-x^{2}/8.}
Quadratic example
[edit ]Consider the expression:
- {\displaystyle (1+\epsilon )^{n}-(1-\epsilon )^{-n}}
where {\displaystyle |\epsilon |<1} and {\displaystyle |n\epsilon |\ll 1}. If only the linear term from the binomial approximation is kept {\displaystyle (1+x)^{\alpha }\approx 1+\alpha x} then the expression unhelpfully simplifies to zero
- {\displaystyle {\begin{aligned}(1+\epsilon )^{n}-(1-\epsilon )^{-n}&\approx (1+n\epsilon )-(1-(-n)\epsilon )\\&\approx (1+n\epsilon )-(1+n\epsilon )\\&\approx 0.\end{aligned}}}
While the expression is small, it is not exactly zero. So now, keeping the quadratic term:
- {\displaystyle {\begin{aligned}(1+\epsilon )^{n}-(1-\epsilon )^{-n}&\approx \left(1+n\epsilon +{\frac {1}{2}}n(n-1)\epsilon ^{2}\right)-\left(1+(-n)(-\epsilon )+{\frac {1}{2}}(-n)(-n-1)(-\epsilon )^{2}\right)\\&\approx \left(1+n\epsilon +{\frac {1}{2}}n(n-1)\epsilon ^{2}\right)-\left(1+n\epsilon +{\frac {1}{2}}n(n+1)\epsilon ^{2}\right)\\&\approx {\frac {1}{2}}n(n-1)\epsilon ^{2}-{\frac {1}{2}}n(n+1)\epsilon ^{2}\\&\approx {\frac {1}{2}}n\epsilon ^{2}((n-1)-(n+1))\\&\approx -n\epsilon ^{2}\end{aligned}}}
This result is quadratic in {\displaystyle \epsilon } which is why it did not appear when only the linear terms in {\displaystyle \epsilon } were kept.
References
[edit ]- ^ For example calculating the multipole expansion. Griffiths, D. (1999). Introduction to Electrodynamics (Third ed.). Pearson Education, Inc. pp. 146–148.