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Mathematical Methods for Physicists: A concise introduction - Site Map

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FUNCTIONS OF A COMPLEX VARIABLE<br />

We may imagine them as lying on a circle of unit radius in the complex plane.<br />

Special points on this circle are<br />

ˆ 0<br />

ˆ =2<br />

ˆ <br />

…1†<br />

ˆ=2<br />

…i†<br />

…1†<br />

…i†:<br />

The reader should know these points at all times.<br />

Sometimes it is easier to use the polar <strong>for</strong>m in manipulations. For example, to<br />

multiply two complex numbers, we multiply their moduli and add their phases; to<br />

divide, we divide by the modulus and subtract the phase of the denominator:<br />

zz 1 ˆ…re i †…r 1 e i 1<br />

†ˆrr 1 e i…‡ 1† ;<br />

z<br />

ˆ rei<br />

z 1 r 1 e i ˆ r e i…1† :<br />

1 r 1<br />

On the other hand to add two complex numbers we have to go back to the<br />

Cartesian <strong>for</strong>ms, add the components and revert to the polar <strong>for</strong>m.<br />

If we view a complex number z as a vector, then the multiplication of z by e i<br />

(where is real) can be interpreted as a rotation of z counterclockwise through<br />

angle ; and we can consider e i as an operator which acts on z to produce this<br />

rotation. Similarly, the multiplication of two complex numbers represents a rotation<br />

and a change of length: z 1 ˆ r 1 e i 1<br />

; z 2 ˆ r 2 e i 2<br />

, z 1 z 2 ˆ r 1 r 2 e i… 1‡ 2 † ; the new<br />

complex number has length r 1 r 2 and phase 1 ‡ 2 .<br />

Example 6.1<br />

Find …1 ‡ i† 8 .<br />

Solution: We<br />

p<br />

®rst write z in polar <strong>for</strong>m: z ˆ 1 ‡ i ˆ r…cos ‡ i sin †, from which<br />

we ®nd r ˆ<br />

<br />

2 ;ˆ =4. Then<br />

p<br />

z ˆ<br />

<br />

p<br />

2 … cos =4 ‡ i sin =4†<br />

ˆ 2 e i=4 :<br />

Thus<br />

p<br />

…1 ‡ i† 8 ˆ… 2 e i=4 † 8 ˆ 16e 2i ˆ 16:<br />

Example 6.2<br />

Show that<br />

p<br />

1 ‡ !<br />

3 i<br />

p<br />

10ˆ<br />

1 1 p<br />

3 i 2 ‡ i 3<br />

2 :<br />

236

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