What is the significance of the number e and Euler's formula?

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Right. So, after some investigation, I have found that there are two looser definitions one might use:

Definition 1:
[itex]\exp(z)[/itex] is the unique function over [itex]\mathbb{C}[/itex] such that:

1. [itex]\frac{d}{dz}(\exp(z))[/itex] exists, and

2. [itex]\exp(x+i0) = e^x[/itex] for all real numbers x.

Definition 2
[itex]\exp(z)[/itex] is the unique function over [itex]\mathbb{C}[/itex] such that:

1. [itex]\frac{d}{dz}(\exp(z)) = \exp(z)[/itex], and

2. [itex]\exp(0) = 1[/itex].

Either definition is sufficient, and they are equivalent.
 
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I was bored in class so I did this, don't really know if it's any use here, but I think so and found it very interesting:

d/dx[exp(x)]=lim h->0 [tex]\frac{exp(x+h)-exp(x)}{h}[/tex] = exp(x) lim h->0 [tex]\frac{exp(h)-1}{h}[/tex]=exp(x) lim h->0 [tex]\frac{\sum\frac{h^k}{k!}-1}{h}[/tex], with the sum from 0 to infinity,

= exp(x) lim h->0 [tex]\frac{\sum\frac{h^k}{k!}}{h}[/tex], with the sum from 1 to infinity

= exp(x) lim h->0 [tex]\sum\frac{h^{(k-1)}}{k!}[/tex]

and all terms in the sum go to zero, except the first, which goes to 1... so:

= exp(x)

so, when you define exp(x) by [tex]\sum\frac{x^k}{k!}[/tex], the deravative of exp(x) is exp(x)
 
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Yes, and that result would have been much easier if you differentiated the series directly, term by term. Or even if you used the limit definition, at the point [tex]\lim_{h\to 0} \frac{e^h -1}{h}[/tex] you could have replaced with the series definition there, subtract one from it and then divide by h, you have the same series again.
 
well that's what I did >_>, at least the second thing.
 
have you studied linear algebra? an "eigenvector" for a linear operator T is a vector v such that Tv is a scalar multiple of v. These vectors provide the most natural coordinate system appropriate to the operator T. If one wants to solve an equation like TX = Y, for X, it is easy to do if Y is expanded in terms of eigenvectors of T.

The functions e^ax provide the eigenvectors for the linear operator D (differentiation). Using them, one gets the most natural expansion of a smooth function, its Fourier series. this makes it easy to solve differential equations like Df = g, if one can expand g in a Fourier series.
 
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I will point out, again, that there is nothing all that magical about e. Any exponential function akx is an eigenfunction of the derivative operator.
 
well there is something special about the eigenvalue 1. or is your point that we should say "fixed points" of the operator D, to characterize ce^x?

i.e. e^x is the unique solution of the primordial ode: Dy = y, y(0) = 1.
 
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