Functional Differential Geometry
.
3.2.1
Instead, the ordinary directional derivative is
or
3.2.2
The first generalization of directional derivative is replacing
, a vector independent of
, with
, a vector function of
.
1. Note that
Instead,
2. The physical meaning of is given by:
p. 25
The function
is the coefficient function for the vector field
. It provides a scale factor for the component in each coordinate direction.
3.
(define (components->vector-field components coordsys) (define (v f) (compose (* (D (compose f (point coordsys))) components) (chart coordsys))) (procedure->vector-field v)) (define R2->R (-> (UP Real Real) Real)) (define R2-rect-chi-inverse (point R2-rect)) (define R2-rect-point (R2-rect-chi-inverse (up 'x_0 'y_0))) (define v (components->vector-field (up (literal-function 'b^0 R2->R) (literal-function 'b^1 R2->R)) R2-rect)) ((v (literal-manifold-function 'f_rect R2-rect)) R2-rect-point)

(define v (literal-vector-field 'b R2-rect)) ((v (literal-manifold-function 'f_rect R2-rect)) R2-rect-point)
4. Eq. (3.7):
p. 25
The vector field
has a coordinate representation
:
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with the definitions
and
.
(define (coordinatize v coordsys) (define ((coordinatized-v f) x) (let ((b (compose (v (chart coordsys)) (point coordsys)))) (* ((D f) x) (b x)))) (make-operator coordinatized-v)) (((coordinatize v R2-rect) (literal-function 'f_rect R2->R)) (up 'x_0 'y_0))
— Me@2024-09-02 01:06:17 AM
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2024.09.03 Tuesday (c) All rights reserved by ACHK
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