Equivalence of Exponential Definitions

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Theorem

All the definitions of the exponential function are equivalent.

$(1): \quad y = \exp x \iff \ln y = x$:
$\quad \quad \ln y = \displaystyle \int_{t=1}^{t=y} \frac 1 t \ \mathrm dt$


$(2): \quad \exp x = e^x$


$(3): \quad \exp x = \displaystyle \lim_{n \to \infty} \left({1 + \frac x n}\right)^n$


$(4): \quad \exp x = \displaystyle \sum_{n = 0}^\infty \frac {x^n} {n!}$


$(5): \quad y = f\left({x}\right)$: $y = \dfrac {\mathrm dy}{\mathrm dx}$, $f\left({0}\right) = 1$


Proof

1 implies 5

\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle x\) \(=\) \(\displaystyle \ln y\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle \int_{t=1}^{t=y} \frac 1 t \ \mathrm dt\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle D_y \left({x}\right)\) \(=\) \(\displaystyle D_y \int_{t=1}^{t=y} \frac 1 t \ \mathrm dt\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          differentiate WRT $y$          
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \frac {\mathrm dx}{\mathrm dy}\) \(=\) \(\displaystyle \frac 1 y\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          Fundamental Theorem of Calculus/First Part          
\(\displaystyle \) \(\displaystyle \iff\) \(\displaystyle \) \(\displaystyle \frac {\mathrm dy}{\mathrm dx}\) \(=\) \(\displaystyle y\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          Derivative of an Inverse Function          

This proves that $y$ is a solution.

Now, let's check if it fulfills the initial condition.

\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle f\left({0}\right)\) \(=\) \(\displaystyle 1\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \iff\) \(\displaystyle \) \(\displaystyle f^{-1}\left({1}\right)\) \(=\) \(\displaystyle 0\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          Inverse Mapping Image          
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \ln y \vert_{y=1}\) \(=\) \(\displaystyle \int_{t=1}^{t=1} \frac 1 t \ \mathrm dt\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle 0\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          Integral on Zero Interval          

... indeed it does.

$\blacksquare$


5 implies 1

\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \frac {\mathrm dy}{\mathrm dx}\) \(=\) \(\displaystyle y\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \iff\) \(\displaystyle \) \(\displaystyle \frac {\mathrm dx}{\mathrm dy}\) \(=\) \(\displaystyle \frac 1 y\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          Derivative of an Inverse Function          
\(\displaystyle \) \(\displaystyle \implies\) \(\displaystyle \) \(\displaystyle \int \ \mathrm dx\) \(=\) \(\displaystyle \int \frac 1 y \ \mathrm dy\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          Separation of Variables          
\(\displaystyle \) \(\displaystyle \implies\) \(\displaystyle \) \(\displaystyle x + C\) \(=\) \(\displaystyle \int_{t=1}^{t=y}\frac 1 t \ \mathrm dt\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          Fundamental Theorem of Calculus/Second Part          

Now to solve for $C$, put $\left(x_0,y_0\right) = \left(0,1\right)$:

\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle 0 + C\) \(=\) \(\displaystyle \int_{t=1}^{t=1}\frac 1 t \ \mathrm dt\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \implies\) \(\displaystyle \) \(\displaystyle C\) \(=\) \(\displaystyle 0\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          Integral on Zero Interval          

$\blacksquare$


1 implies 3

We have:

\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \ln \left({\left({1 + \frac x n}\right)^n}\right)\) \(=\) \(\displaystyle n \ln \left({1 + xn^{-1} }\right)\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          Logarithms of Powers          
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle x \frac {\ln \left({1 + x n^{-1} }\right)} {x n^{-1} }\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          multiply by $1 = \dfrac { xn^{-1} }{ xn^{-1} }$          

From Limit of Sequence is Limit of Real Function, we can consider the differentiable analogue of the sequence.

From Derivative of Logarithm at One we have:

$\displaystyle \lim_{x \to 0} \frac {\ln \left({1 + x}\right)} x = 1$


But $x n^{-1} \to 0$ as $n \to \infty$ from Power of Reciprocal.

Thus:

$\displaystyle x \frac {\ln \left({1 + x n^{-1}}\right)} {x n^{-1}} \to x$

as $n \to \infty$.


Since the exponential function is continuous at every point, it follows that:

$\displaystyle \left({1 + \frac x n}\right)^n = \exp \left({n \ln \left({1 + \frac x n}\right)}\right) \to \exp x = e^x$

as $n \to \infty$.

$\blacksquare$


5 implies 4

From Higher Derivatives of Exponential Function, we have:

$\forall n \in \N: f^{\left({n}\right)} \left({\exp x}\right) = \exp x$


Since $\exp 0 = 1$, the Taylor series expansion for $\exp x$ about $0$ is given by:

$\displaystyle \exp x = \sum_{n=0}^\infty \frac {x^n} {n!}$


From Power Series over Factorial, we know that this power series expansion converges for all $x \in \R$.

From Taylor's Theorem, we know that

$\displaystyle \exp x = 1 + \frac {x} {1!} + \frac {x^2} {2!} + \cdots + \frac {x^{n-1}} {\left({n-1}\right)!} + \frac {x^n} {n!} \exp \left({\eta}\right)$

where $0 \le \eta \le x$.

Hence:

\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \left \vert {\exp x - \left({1 + \frac x {1!} + \frac {x^2} {2!} + \cdots + \frac {x^{n-1} } {\left({n-1}\right)!} }\right)} \right \vert\) \(=\) \(\displaystyle \left \vert {\frac {x^n} {n!} \exp \left({\eta}\right)} \right \vert\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\le\) \(\displaystyle \frac {\left \vert {x^n} \right \vert} {n!} \exp \left({\left \vert {x} \right \vert}\right)\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\to\) \(\displaystyle 0 \text { as } n \to \infty\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          by Series of Power over Factorial Converges          


So the partial sums of the power series converge to $\exp x$.

The result follows.

$\blacksquare$


3 implies 4

From the Binomial Theorem:

$\displaystyle \left({1 + \frac x n}\right)^n = 1 + x + \frac{n\left({n-1}\right)x^2}{2! \ n^2} + \frac{n\left({n-1}\right)\left({n-2}\right)x^3}{3! \ n^3} + \cdots$
$ = \displaystyle \frac {x^0}{0!} + \frac {x^1}{1!} + \left({\frac {n-1} {n} }\right) \frac {x^2}{2!} + \left({{\frac {\left({n-1}\right)\left({n-2}\right)} {n^2} }}\right) \frac {x^3}{3!} + \cdots$
\(\displaystyle \) \(\displaystyle \implies\) \(\displaystyle \) \(\displaystyle \left({1 + \frac x n}\right)^n - \frac {x^0}{0!} + \frac {x^1}{1!} + \left({\frac {n-1} {n} }\right) \frac {x^2}{2!} + \left({{\frac {\left({n-1}\right)\left({n-2}\right)} {n^2} }}\right) \frac {x^3}{3!} + \cdots\) \(=\) \(\displaystyle 0\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    

From Power of a Number Less Than One, this converges to:

$\displaystyle \exp x - \frac {x^0}{0!} + \frac {x^1}{1!} + \frac {x^2}{2!} + \frac {x^3}{3!} + \cdots = 0$

as $n \to +\infty$

\(\displaystyle \) \(\displaystyle \implies\) \(\displaystyle \) \(\displaystyle \exp x\) \(=\) \(\displaystyle \sum_{n = 0}^\infty \frac {x^n} {n!}\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    

$\blacksquare$

Compare Series of Power over Factorial Converges.


4 implies 5

\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \dfrac {\mathrm d}{\mathrm dx}\sum_{n = 0}^\infty \frac {x^n} {n!}\) \(=\) \(\displaystyle \dfrac {\mathrm d}{\mathrm dx} \left({\frac {x^0}{0!} + \frac {x^1}{1!} + \frac {x^2}{2!} + \frac {x^3}{3!} + \cdots } \right)\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle 0 + 1 + \frac {2x} {2 \cdot 1} + \frac {3x}{3 \cdot 2 \cdot 1} + \cdots\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle \frac {x^0}{0!} + \frac {x^1}{1!} + \frac {x^2}{2!} + \frac {x^3}{3!} + \cdots\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle \sum_{n = 0}^\infty \frac {x^n} {n!}\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \sum_{n = 0}^\infty \frac {0^n} {n!}\) \(=\) \(\displaystyle \frac {0^0} {0!} + 0 + 0 + \cdots\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle 1\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          definition of $0^0$          

$\blacksquare$

3 implies 2

Let the restriction of the exponential function to the rationals be defined as:

$\exp \restriction_{\Q}: x \mapsto \displaystyle \lim_{n \to +\infty}\left (1 + \frac x n\right)^n$

Let $e$ be Euler's Number defined as:

$e = \displaystyle \lim_{n \to +\infty}\left (1 + \frac 1 n\right)^n$


For $x=0$:

\(\displaystyle \) \(\displaystyle \exp \restriction_{\Q} \ 0\) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle \lim_{n \to +\infty}\left (1 + \frac 0 n\right)^n\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle 1\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle e^0\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    

$\Box$

For $x \ne 0$:

\(\displaystyle \) \(\displaystyle \exp \restriction_{\Q} \ x\) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle \lim_{n \to +\infty}\left (1 + \frac x n\right)^n\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle \lim_{\left({n/x}\right) \to +\infty}\left (\left (1 + \frac 1 { \left({n/x}\right) } \right)^{\left({n/x}\right)}\right)^x\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          Exponent Combination Laws          
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle e^x\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    

$\blacksquare$


3 implies 5

\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle D_x \left({\exp x}\right)\) \(=\) \(\displaystyle \lim_{h \to 0} \frac {\exp \left({x+h}\right) - \exp x} h\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          by definition of derivative          
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle \lim_{h \to 0} \frac {\exp x \cdot \exp h - \exp x} h\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          Exponent of Sum          
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle \lim_{h \to 0} \frac {\exp x \left({\exp h - 1}\right)} h\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle \exp x \left({\lim_{h \to 0} \frac {\exp h - 1} h}\right)\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          Multiple Rule for Limits of Functions, as $\exp x$ is constant          
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle \exp x\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          Derivative of Exponential at Zero          


The application of Derivative of Exponential at Zero isn't circular as the referenced proof does not depend on $D_x \exp x = \exp x$.

$\Box$

\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \exp 0\) \(=\) \(\displaystyle \lim_{n \to +\infty} \left({1 + \frac 0 n}\right)^n\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle 1\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    

$\blacksquare$


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