Subject:	dedanoe's levers in rescue of string theory
Date:	Sat, 5 Dec 2009 09:55:10 -0800 (PST)

this is Bezier's adaptation of the lever law:

string in 2d:

| P1 P2 |
| | = P
| t 1-t|

with t in [0, 1]

string in 3d:

| P1 P2 P3 |
| t^2 (1-t)^2 2(1-t)t| = P
|2(1-s)s s^2 (1-s)^2|

with t, s in [0, 1]

string in 4d:

| P1 P2 P3 P4 |
| t^3 (1-t)^3 3(1-t)^2 t 3(1-t) t^2|
| | = P
|3(1-s) s^2 s^3 (1-s)^3 3(1-s)^2 s|
|3(1-k)^2 k 3(1-k) k^2 k^3 (1-k)^3 |

with t, s, k in [0, 1]
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
P1, P2, P3, P4 are the local weights and
P is their equipotential weight or the string of the lever.

i am willing to negotiate the acceptance of this claim

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