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Lecture Notes in Differential Equations - Bruce E. Shapiro

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155<br />

Theorem 18.2. Euler’s Formula<br />

e iθ = cos θ + i s<strong>in</strong> θ (18.18)<br />

Proof. Use the fact that<br />

⎫ ⎧<br />

i 2 = −1<br />

i 4k+1 ⎫<br />

= i<br />

i 3 = i(i 2 ) = −i<br />

⎪⎬ ⎪⎨ i 4k+2 = −1<br />

⎪⎬<br />

=⇒<br />

i 4 = i(i 3 ) = i(−i) = 1 i 4k+3 = −i<br />

⎪⎭ ⎪⎩<br />

⎪⎭<br />

i 5 = i(i 4 ) = i<br />

i 4k+4 = 1<br />

<strong>in</strong> the formula’s for a Taylor Series of e iθ :<br />

for all k = 0, 1, 2, . . .<br />

(18.19)<br />

e iθ = 1 + (iθ) + (iθ)2<br />

2!<br />

= 1 + iθ + i2 θ 2<br />

=<br />

2!<br />

+ (iθ)3<br />

3!<br />

+ i3 θ 3<br />

3!<br />

+ i4 θ 4<br />

4!<br />

+ (iθ)4<br />

4!<br />

+ i5 θ 5<br />

5!<br />

+ (iθ)5<br />

5!<br />

+ · · · (18.20)<br />

+ · · · (18.21)<br />

= 1 + iθ − θ2<br />

2! + −iθ3 3! + θ4<br />

4! + iθ5 5! + · · · (18.22)<br />

even powers of θ<br />

{ }} {<br />

(1 − θ2<br />

2! + θ4<br />

4! − θ6<br />

6! + · · · )<br />

+i<br />

(θ − θ3<br />

)<br />

3! + θ5<br />

5! − θ7<br />

7! + · · · } {{ }<br />

odd powers of θ<br />

(18.23)<br />

= cos θ + i s<strong>in</strong> θ (18.24)<br />

where the last step follows because we have used the Taylor series for s<strong>in</strong> θ<br />

and cos θ.<br />

Theorem 18.3. If z = a + ib where a and b are real numbers than<br />

e z = e a+ib = e a (cos θ + i s<strong>in</strong> θ) (18.25)<br />

Theorem 18.4. If z = x + iy where x, y are real, then<br />

where θ = Phase(z) and r = |z|.<br />

z = r(cos θ + i s<strong>in</strong> θ) = re iθ (18.26)<br />

Proof. By def<strong>in</strong>ition θ = Phase(z) is the angle between the x axis and the

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