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ForwardTheory-> exp_forward log_forward sqrt_forward sin_cos_forward atan_forward asin_forward acos_forward tan_forward erf_forward

exp_forward

Headings-> Derivatives Taylor Coefficients Recursion

@(@\newcommand{\W}[1]{ \; #1 \; } \newcommand{\R}[1]{ {\rm #1} } \newcommand{\B}[1]{ {\bf #1} } \newcommand{\D}[2]{ \frac{\partial #1}{\partial #2} } \newcommand{\DD}[3]{ \frac{\partial^2 #1}{\partial #2 \partial #3} } \newcommand{\Dpow}[2]{ \frac{\partial^{#1}}{\partial {#2}^{#1}} } \newcommand{\dpow}[2]{ \frac{ {\rm d}^{#1}}{{\rm d}\, {#2}^{#1}} }@)@Exponential Function Forward Mode Theory
Derivatives
If @(@ F(x) @)@ is @(@ \R{exp} (x) @)@ or @(@ \R{expm1} (x) @)@ the corresponding derivative satisfies the equation @[@ 1 * F^{(1)} (x) - 1 * F (x) = d^{(0)} = \left\{ \begin{array}{ll} 0 & \R{if} \; F(x) = \R{exp}(x) \\ 1 & \R{if} \; F(x) = \R{expm1}(x) \end{array} \right. @]@ where the equation above defines @(@ d^{(0)} @)@. In the standard math function differential equation , @(@ A(x) = 1 @)@, @(@ B(x) = 1 @)@, and @(@ D(x) = d^{(0)} @)@. We use @(@ a @)@, @(@ b @)@, @(@ d @)@, and @(@ z @)@ to denote the Taylor coefficients for @(@ A [ X (t) ] @)@, @(@ B [ X (t) ] @)@, @(@ D [ X (t) ] @)@, and @(@ F [ X(t) ] @)@ respectively.

Taylor Coefficients Recursion
For orders @(@ j = 0 , 1, \ldots @)@, @[@ \begin{array}{rcl} z^{(0)} & = & F ( x^{(0)} ) \\ e^{(0)} & = & d^{(0)} + z^{(0)} \\ e^{(j+1)} & = & d^{(j+1)} + \sum_{k=0}^{j+1} a^{(j+1-k)} * z^{(k)} \\ & = & z^{(j+1)} \\ z^{(j+1)} & = & \frac{1}{j+1} \frac{1}{ b^{(0)} } \left( \sum_{k=1}^{j+1} k x^{(k)} e^{(j+1-k)} - \sum_{k=1}^j k z^{(k)} b^{(j+1-k)} \right) \\ & = & x^{(j+1)} d^{(0)} + \frac{1}{j+1} \sum_{k=1}^{j+1} k x^{(k)} z^{(j+1-k)} \end{array} @]@

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Input File: omh/appendix/theory/exp_forward.omh