Solving PDF Integrals of Normal Distribution

Solving PDF Integrals of Normal Distribution


normal distribution statistics

We know that a random variable distribution must satisfy the fundamental probability density function (PDF) requirements for a continuous random variable:

  1. f(x)0f(x) \geq 0, for all xRx \in \mathbb{R}

  2. f(x)dx=1\int_{-\infty}^{\infty} f(x)\,dx = 1

  3. P(a<X<b)=abf(x)dxP(a < X < b) = \int_a^b f(x)\,dx

These conditions ensure that the function is a valid probability model over the continuous sample space.


To prove that the total area under the normal distribution curve is equal to 1, we evaluate:

P(<X<)=f(x)dxP(-\infty < X < \infty) = \int_{-\infty}^{\infty} f(x)\,dx

Substituting the normal distribution PDF:

=1σ2πe(xμ)22σ2dx= \int_{-\infty}^{\infty} \frac{1}{\sigma\sqrt{2\pi}} e^{-\frac{(x-\mu)^2}{2\sigma^2}} dx

Standardization Transformation

Let:

z=xμσz = \frac{x-\mu}{\sigma}

Then:

x=σz+μx = \sigma z + \mu dx=σdzdx = \sigma dz

Substituting:

=1σ2πe(σz+μμ)22σ2σdz= \int_{-\infty}^{\infty} \frac{1}{\sigma\sqrt{2\pi}} e^{-\frac{(\sigma z + \mu - \mu)^2}{2\sigma^2}} \sigma dz

Simplifying:

=12πez22dz= \int_{-\infty}^{\infty} \frac{1}{\sqrt{2\pi}} e^{-\frac{z^2}{2}} dz =12πez2/2dz= \frac{1}{\sqrt{2\pi}} \int_{-\infty}^{\infty} e^{-z^2/2} dz

Relating to the Gaussian Integral

Recall:

ey2dy=π\int_{-\infty}^{\infty} e^{-y^2}\,dy = \sqrt{\pi}

To match this form, let:

y=z2y = \frac{z}{\sqrt{2}}

Then:

z=2yz = \sqrt{2}y dz=2dydz = \sqrt{2}\,dy

Substituting:

=12πe(2y)2/22dy= \frac{1}{\sqrt{2\pi}} \int_{-\infty}^{\infty} e^{-(\sqrt{2}y)^2/2} \sqrt{2}\,dy

Simplifying:

=1πey2dy= \frac{1}{\sqrt{\pi}} \int_{-\infty}^{\infty} e^{-y^2} dy

Using the Gaussian integral result:

=1ππ= \frac{1}{\sqrt{\pi}} \cdot \sqrt{\pi} =1= 1

Final Result

P(<X<)=f(x)dx=1P(-\infty < X < \infty) = \int_{-\infty}^{\infty} f(x)\,dx = 1

Thus, it is proven that the total area under the normal distribution curve is exactly 1, satisfying the fundamental requirement of a valid probability density function.