This namespace implements a number of differential operators like D
, and
the machinery to apply D
to various structures.
This namespace implements a number of differential operators like [[D]], and the machinery to apply [[D]] to various structures.
Derivative operator. Takes some function f
and returns a function
whose value at some point can multiply an increment in the arguments, to
produce the best linear estimate of the increment in the function value.
For univariate functions, D
computes a derivative. For vector-valued
functions, D
computes
the Jacobian
of f
.
The related [[Grad]] returns a function that produces a structure of the
opposite orientation as D
. Both of these functions use forward-mode
automatic differentiation.
Derivative operator. Takes some function `f` and returns a function whose value at some point can multiply an increment in the arguments, to produce the best linear estimate of the increment in the function value. For univariate functions, [[D]] computes a derivative. For vector-valued functions, [[D]] computes the [Jacobian](https://en.wikipedia.org/wiki/Jacobian_matrix_and_determinant) of `f`. The related [[Grad]] returns a function that produces a structure of the opposite orientation as [[D]]. Both of these functions use forward-mode automatic differentiation.
(derivative f)
Returns a single-argument function of that, when called with an argument x
,
returns the derivative of f
at x
using forward-mode automatic
differentiation.
For numerical differentiation,
see emmy.numerical.derivative/D-numeric
.
f
must be built out of generic operations that know how to
handle [[d/Differential]] inputs in addition to any types that a normal (f x)
call would present. This restriction does not apply to operations like
putting x
into a container or destructuring; just primitive function calls.
Returns a single-argument function of that, when called with an argument `x`, returns the derivative of `f` at `x` using forward-mode automatic differentiation. For numerical differentiation, see [[emmy.numerical.derivative/D-numeric]]. `f` must be built out of generic operations that know how to handle [[d/Differential]] inputs in addition to any types that a normal `(f x)` call would present. This restriction does _not_ apply to operations like putting `x` into a container or destructuring; just primitive function calls.
(partial & selectors)
Returns an operator that, when applied to a function f
, produces a function
that computes the partial derivative of f
at the (zero-based) slot index
provided via selectors
.
Returns an operator that, when applied to a function `f`, produces a function that computes the partial derivative of `f` at the (zero-based) slot index provided via `selectors`.
(symbolic-taylor-series f)
(symbolic-taylor-series f & xs)
Similar to taylor-series
, except f
is evaluated with symbolic arguments,
and these arguments are only replaced with the values xs
after Taylor series
expansion.
Please see the docs for taylor-series
!
Similar to [[taylor-series]], except `f` is evaluated with symbolic arguments, and these arguments are only replaced with the values `xs` after Taylor series expansion. Please see the docs for [[taylor-series]]!
(taylor-series f)
(taylor-series f & xs)
Given a differentiable function f
and any number of arguments xs
, returns
a [[emmy.series/PowerSeries]] representing the Taylor
series of the function f
expanded at xs
.
Calling taylor-series
with no arguments will return the Maclaurin
series
of f
, i.e., the Taylor series expansion at (= x 0)
.
Calling the returned power series with incremental argument dx
will produce
a [[emmy.series/Series]] representing the terms of the Taylor series of
f
expanded at x
and evaluated at x+dx
.
NOTE: Just like the D
operator, functions f
of multiple-arguments are
treated as a function of a single structural argument. If you pass multiple
arguments xs
, you'll have to manually wrap your multiple-argument dx
in
a emmy.structure/up
or a vector before passing it to the returned
power series.
NOTE: The typical definition of a Taylor series of f
expanded around some
point x
is
$$T(p) = f(x) + \frac{f'(x)}{1!}(p-x) + \frac{f''(x)}{2!} (p-x)^2 + \ldots,$$
where p
is the evaluation point. When (= p x)
, all derivatives of the
Taylor series expansion of f
will exactly match the derivatives of f
itself.
The Taylor series returned here (call it $T'$) is actually a function of dx
,
where
$$T'(dx) = T(x+dx) = f(x) + \frac{f'(x)}{1!}(dx) + \frac{f''(x)}{2!} (dx)^2 + \ldots.$$
Given a differentiable function `f` and any number of arguments `xs`, returns a [[emmy.series/PowerSeries]] representing the [Taylor series](https://en.wikipedia.org/wiki/Taylor_series) of the function `f` expanded at `xs`. Calling [[taylor-series]] with no arguments will return the [Maclaurin series](https://en.wikipedia.org/wiki/Taylor_series#List_of_Maclaurin_series_of_some_common_functions) of `f`, i.e., the Taylor series expansion at `(= x 0)`. Calling the returned power series with incremental argument `dx` will produce a [[emmy.series/Series]] representing the terms of the Taylor series of `f` expanded at `x` and evaluated at `x+dx`. NOTE: Just like the [[D]] operator, functions `f` of multiple-arguments are treated as a function of a single structural argument. If you pass multiple arguments `xs`, you'll have to manually wrap your multiple-argument `dx` in a [[emmy.structure/up]] or a vector before passing it to the returned power series. NOTE: The typical definition of a Taylor series of `f` expanded around some point `x` is $$T(p) = f(x) + \frac{f'(x)}{1!}(p-x) + \frac{f''(x)}{2!} (p-x)^2 + \ldots,$$ where `p` is the evaluation point. When `(= p x)`, all derivatives of the Taylor series expansion of `f` will exactly match the derivatives of `f` itself. The Taylor series returned here (call it $T'$) is actually a function of `dx`, where $$T'(dx) = T(x+dx) = f(x) + \frac{f'(x)}{1!}(dx) + \frac{f''(x)}{2!} (dx)^2 + \ldots.$$
cljdoc is a website building & hosting documentation for Clojure/Script libraries
× close