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ONT Re: Differential Logic




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DLOG.  Note D59

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Remainder of Conjunction

| I bequeath myself to the dirt to grow from the grass I love,
| If you want me again look for me under your bootsoles.
|
| You will hardly know who I am or what I mean,
| But I shall be good health to you nevertheless,
| And filter and fibre your blood.
|
| Failing to fetch me at first keep encouraged,
| Missing me one place search another,
| I stop some where waiting for you
|
| Walt Whitman, 'Leaves of Grass', [Whi, 88]

Let us now recapitulate the story so far.  In effect, we have
been carrying out a decomposition of the enlarged proposition
EJ in a series of stages.  First, we considered the equation
EJ = !e!J + DJ, which was involved in the definition of DJ as
the difference EJ - !e!J.  Next, we contemplated the equation
DJ = dJ + rJ, which expresses DJ in terms of two components,
the differential dJ that was just extracted and the residual
component rJ = DJ - dJ.  This remaining proposition rJ can
be computed as shown in Table 47.

Table 47.  Computation of rJ
o-------------------------------------------------------------------------------o
|                                                                               |
| rJ  =        DJ        +        dJ                                            |
|                                                                               |
o-------------------------------------------------------------------------------o
|                                                                               |
| DJ  =  u v ((du)(dv))  +   u (v)(du) dv   +  (u) v  du (dv)  +  (u)(v) du dv  |
|                                                                               |
| dj  =  u v  (du, dv)   +   u (v) dv       +  (u) v  du       +  (u)(v) . 0    |
|                                                                               |
o-------------------------------------------------------------------------------o
|                                                                               |
| rJ  =  u v   du  dv    +   u (v) du  dv   +  (u) v  du  dv   +  (u)(v) du dv  |
|                                                                               |
o-------------------------------------------------------------------------------o

As it happens, the remainder rJ falls under the description
of a second order differential rJ = d^2.J.  This means that
the expansion of EJ in the form:

   EJ   =   !e!J    +   DJ

        =   !e!J    +   dJ      +   rJ

        =   d^0.J   +   d^1.J   +   d^2.J

which is nothing other than the propositional analogue
of a Taylor series, is a decomposition that terminates
in a finite number of steps.

Jon Awbrey

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