Euler's Relation Explained - No Derivation Needed

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In summary, Euler derived the formula exp(j*)=cos*+jsin* without going into his actual derivation. He used series expansion and showed that they were equal.
  • #1
ragavcit
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Hello everyone,
Can anyone give me a brief explanation about how EULER derived the formula exp(j*)=cos*+jsin* without going into his actual derivation..
 
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  • #2
I'm not sure exactly how Euler did it, but a simple way to do it is to write out the taylor series for both sides of the equation and showing that they are equal.
 
  • #3
I think Euler used series expansion. This result is not really derived though, since it is the extension of the definition into a larger domain. Usually several properties of
exp:R->R
are chosen to be preserved in the extension
exp:C->C
and the formula folows naturally
I like preserving these properties
exp(a+b)=exp(a)*exp(b)
and
lim_{x->0}[exp(x)-1]/x=1
 
  • #4
Euler did use the series expansion, plugging in [itex]\theta := i\theta[/tex] in the defining series for the exponential,

[tex]\exp{\theta} = \sum_{n = 0}^{+\infty} \frac{\theta^{n}}{n!}[/tex]

and seperating real and imaginary parts. It was a phenomenal achievement in the true Eulerian spirit. A bit of a shame that people overlook this 'derivation' entirely and choose to define the exponential from scratch nowadays.
 
  • #5
yasiru89 said:
A bit of a shame that people overlook this 'derivation' entirely and choose to define the exponential from scratch nowadays.
It is overlooked because it is not a 'derivation'. You cannot 'derive' an identity of a function without first giving a definition of the function. It is possible to extend the real exponential to the complex plane by analytic continuation, and this is done in introductory books with titles like analysis or complex variables. The approach involves Heavy lifting.
 
  • #6
lurflurf said:
It is overlooked because it is not a 'derivation'. You cannot 'derive' an identity of a function without first giving a definition of the function. It is possible to extend the real exponential to the complex plane by analytic continuation, and this is done in introductory books with titles like analysis or complex variables. The approach involves Heavy lifting.
This is precisely why I chose to emphasise 'derivation', however, my criticism is not of the analytic extension as such, but of the practice to simply define,

[tex]\exp{it} = \cos{t} + i\sin{t}[/tex].

A better approach is to define the complex analogue as,

[tex]\exp{z} = \sum_{n = 0}^{+\infty} \frac{z^{n}}{n!} [/tex]
, establish global convergence and proceed to show as Euler did that this may be considered to be composed of two components which in themselves may be used to define (or show that they are the corresponding Taylor expansions about the origin of) the cosine and sine functions.
 

FAQ: Euler's Relation Explained - No Derivation Needed

What is Euler's Relation?

Euler's Relation is a mathematical equation that describes the relationship between the trigonometric functions sine, cosine, and tangent in a right triangle. It states that the square of the length of the hypotenuse (the side opposite the right angle) is equal to the sum of the squares of the other two sides.

Who discovered Euler's Relation?

Euler's Relation was discovered by Swiss mathematician Leonhard Euler in the 18th century. It was one of the many contributions he made to the field of mathematics.

How is Euler's Relation useful?

Euler's Relation is useful in solving problems involving right triangles, especially in trigonometry and geometry. It can also be used to derive other important equations, such as the Pythagorean theorem.

Is there a derivation for Euler's Relation?

Yes, there is a mathematical proof for Euler's Relation. It involves using the Pythagorean theorem and basic algebra to show that the equation is true for all right triangles.

Can Euler's Relation be applied to non-right triangles?

No, Euler's Relation only applies to right triangles. It is a special case of the Law of Cosines, which can be used to find the relationship between the sides and angles of any triangle.

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