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The Exponential Integral

Not to be confused with the Exponential Anti-derivative (ie., the integral of exp(z)), the exponential integral, Ei(z), cannot be evaluated in closed form (with finite terms of elementary functions) and, as such, it is a special function. It is surprising when considering the apparent simplicity of the integrands, but the integration does not lead to a trivial solution. Like other special functions, the exponential integral can be evaluated by approximation to an arbitrary accuracy using infinite series. For a more detailed description see Wolfram functions.

Definition

The Exponential Integral is defined by the integral,

E1(x)=-exp(-x)xdx

Series Expansion

The function can be approximation using the series expansion, which is useful for evaluation in software,

E1(z)=-γ-lnz-n=1(-1)nznn!n

Hypergeometric Form

It is possible to express the Exponential integral as a hypergeometric function,

E1(z)=-γ-lnz+ 2F2(1,1;2,2;-z)z

Graph

The Polynomial Denominator

Another useful variant is the integral with a square denominator

exp(-x)x2dx

We can go about evaluating this by finding the exponential integral by integration by parts. Expressing the exponential integral (with x1 in the denominator) in the form,

exp(-x)xdx=uvdx=uv-vudx

We have, u=exp(-x) and v=1x, and so u=-exp(x) and v=-1x2. Hence,

exp(-x)xdx=-exp(-x)x-exp(-x)x2

Now we recognise the integral on the left as being the definition -E1(x), and hence we can solve it for the integral on the right. ie.,

exp(-x)x2dx=E1(x)-exp(-x)x

The Double Integral

Another property which can be useful is the integral of the exponential integral,

exp(-x)xdxdx=E1(x)dx=xE1(x)-exp(-x)