An introduction to Complex numbers

 

 

 

 

Complex numbers and transformations

A transformation on the plane maps each point M to its image M'.
We can then associate each point to its affix. Let’s call these affixes z and z', two complex numbers.

We can now write the transformation in complex terms:

z'=f(z) where f is the complex function associating z to z'

Translation

For a vector \vec{v} we have an affix m.

We can simply write that:

z'=z+m

This simplifies to adding two vectors.

Let’s consider a point A with affix z_A=3+4i
Now let’s translate it using \vec{v}\binom 5{-3}.This is the same as adding it to the complex 5-3i
We get another point A' which is the image of A with affix z_{A'}

z_{A'}=z_A+5-3i
z_{A'}=3+4i+5-3i=8+i

This can be used as a ship’s speed moving it along its course. Very solid concept.

Rotation from a complex number point of view

The Rotation must be centered at the origin O. If \theta is the angle of rotation:
The image of z is

z'=e^{i\theta}z

This was the easiest case. Now, let’s take another center of rotation \Omega with an affix \omega.
The idea is to move the center of rotation to the origin O.This is a simple translation by adding -\omega first and then make the rotation and finally add \omega to take the point to its original position.

z'=e^{i\theta}(z-\omega)+\omega

 

Example:

Simple rotation about O

A point A with affix z_A=1+i is rotated about the origin by \frac{\pi}{4}, find the point A' of affix z_{A'}, image of A after rotation.

z_A=\sqrt{2}(cos \frac{\pi}{4}+ i \sin \frac{\pi}{4}), \frac{\pi}{4} is the base angle.

In exponent expression:
z_A=\sqrt{2}e^{i\frac{\pi}{4}}

We use the rotation formula:
z_{A'}=e^{i\frac{\pi}{4}}z_A=e^{i\frac{\pi}{4}}\cdot \sqrt{2}e^{i\frac{\pi}{4}}=\sqrt{2}e^{i(\frac{\pi}{4}+\frac{\pi}{4})}
z_{A'}=\sqrt{2}e^{i\frac{\pi}{2}}=\sqrt{2}(\cos \frac{\pi}{2}+i\sin \frac{\pi}{2})=i\sqrt{2}

 

Rotation about any point

Now let’s rotate the point A with affix z_A=1+i about another point A point \Omega with affix \omega=2 by \frac{\pi}{4}

we use our formula:
z'=e^{i\theta}(z-\omega)+\omega

z_A-\omega=1+i-2=-1+i

We can see that the resulting image:
z'_A=-1+i=\sqrt{2}(cos \frac{3\pi}{4}+ i \sin \frac{3\pi}{4}), \frac{3\pi}{4} is the base angle.
z''_A=\sqrt{2}e^{i\frac{\pi}{4}}e^{i\frac{3\pi}{4}}+2=\sqrt{2}e^{i(\frac{\pi}{4}+\frac{3\pi}{4})}+2=\sqrt{2}e^{i\pi}+2=2+\sqrt{2}(cos \pi+ i \sin \pi)=2-\sqrt{2}

This is the final image

 

 

 

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