How can I integrate e^(-(x^2)/2)?

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The integral of the function y=e^(-(x^2)/2) does not have an elementary antiderivative, making it challenging to integrate using standard methods like Integration by Parts or Algebraic Substitution. Numerical approximations, such as Simpson's Rule, are typically employed to create Normal Distribution tables. A double integral approach can evaluate the integral from -infinity to infinity, leading to the result that ∫e^(-x^2/2) dx equals √(2π), but it is not effective for finite limits. Various approximation functions exist, with one suggested approximation being e^(-x^2/2) / (1.64x + √(0.76x^2 + 4)). Overall, the discussion emphasizes the complexity of integrating this function and the reliance on numerical methods for practical applications.
prasannapakkiam
I fell very silly posting this, but I am making Normal Distribution tables. I tried to Integrate what seems to be quite a simple function:
y=e^(-(x^2)/2)
Well... I can't I have tried Integration by Parts, Algebraic Substitution etc. But I cannot do it! Can somebody help me?
 
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Ok. But I don't intitutively see why... Can anyone answer this?

So all tables are created as an approximation - e.g. the Simpson's Rule?
 
Yes, they are numerical approximations. I can assure you they weren't calculated via Simpson's Rule.

There is no elementary antiderivative of the pdf. Elementary being sums/products/compositions of 'nice' functions.
 
It can be very hard to prove that a certain function has non-elementary antiderivatives. We know in this case that no known function has its derivative as that integral, so we defined one.
 
prasannapakkiam said:
I fell very silly posting this, but I am making Normal Distribution tables. I tried to Integrate what seems to be quite a simple function:
y=e^(-(x^2)/2)
Well... I can't I have tried Integration by Parts, Algebraic Substitution etc. But I cannot do it! Can somebody help me?
One could do it by numerical integration, but try a double integral, as in

\int_{0}^{x} e^{-x^2} dx\,\int_{0}^{y} e^{-y^2} dy, where I is each integral.

combine the two and use the transformation from Cartesian (x, y) to polar coordinates (r, \theta).

Limits (0,x) and (0, y) become (0, r) and (0, 2\pi)
 
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I am not too sure about Astronuc's suggestion. But anyway, can someone give me a reasonable function for an approximation. So far I have only come up with tanh(x), with a precding constant...
 
Astronuc said:
... but try a double integral, as in...

The double integral method is good for evaluating the definite integral of exp(-x^2/2) from -infinty to infinity, but it is of no use for integrating over finite limits.

The double integral method works by transforming the square of the integral into a double integral over a region of the x,y plane. Since the element of area dx dy becomes r \, dr \, d\theta then it follows that the inner of the two dimensional (dr \, d\theta) integral becomes the trivial \int r e^{-r^2/2} dr.

The catch is that the limits of the integration correspond to a square region of the x,y plane, so r is not a constant! Bascially the difficulty just gets tranferred to the outer d\theta integral, so in general this is no solution.

For the specific case of the integral from -infinity to +infinity however the double integral is over the entire x,y plane and therefore the difficulty with the rectangular limits vanishes. This is the standard method of proving that \int_{-\infty}^{+\infty} e^{-x^2/2} dx = \sqrt{2 \pi}
But anyway, can someone give me a reasonable function for an approximation.
Goolging for 'erf approximations' gives several very good approximations in the first few hits. One nice simple one is :\frac{1}{\sqrt{2 \pi}} \int_x^{\infty} e^{-x^2/2} \, \simeq \frac{ e^{-x^2/2} } {1.64 x + \sqrt{0.76 x^2 + 4}}
 
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I see...
 
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