*I have presented this exactly as I found it; some items referred to in it are missing to date.*

From
the pamphlet:

4th
Conference on Planetology and Space Mission Planning: R.D. and J.M Enzmann,
December 1972

This pamphlet is for the convenience of
the press. Here we have gathered prints of the slides used with the paper on
Order Theory: and included also a diagram of the physics involved in the formation
of star bows. The formation of star-bows takes place when a vehicle moves at
any velocity against the continuum; however it is only markedly developed at
velocities that are a significant fraction of the velocity of light. Star-bows
have been beautifully painted by artist R. Sternbach, as displayed in this session.

(This is a painting by Don Davis showing a star-bow. see also 'Welcome Aboard')

The mathematical background supporting
this release is contained in the accompanying paper. IT has also been published
at:

Trans.AM.Geophyisical Union. Enzmann, RD
and JM, 1972.

*Precession of Planetary Perihelia*. 53:11, page 1110.
Ann. N.Y. Academy of Sciences. Enzmann
RD and JM, and Girard, A. 1972.

*Cosmological Aspects of Order, Relevance, and Information Theory*. 187: page 10.
The accompanying paper is

Enzmann, RD and JM, 1972.

*Order Theory as Applied to Problems of Gravitation.***Gravitational Doppler**

To predict gravitational red or blue
shift you need only:

1) Euclid’s Geometry x y z as f(t)

2) A Newtonian Potential Equation U =
-GMm/R

3) Hasenohrl’s Principle of the Inertia
of Electromagnetic Energy m

_{o }= E/C^{2}Circa 1903
4) Planck’s Equation e = h

*v*

**Gravitational Bending of Light**

To Predict
Gravitational Bending of Light You Need Only:

1) Euclid’s Geometry x y z as f(t)

2) Kepler’s Three Laws of Planetary Motion

3) Newton’s second Law as he stated it F = dp/dt

4) Planck’s Equation e = h

*v*
5) Hasenohrl’s Principle of the Inertia of Electromagnetic Energy m = e

^{2}/c circa 1903**Equivalence is a Statement of Observational Ambiguity, Not a Physical Law, and is Invalid**

**Precession of Planetary Perihelia**

To Predict Precession of
Orbital Perihelia You Need Only:

1) Euclid’s Geometry x y z as f(t)

2) Kepler’s Three Laws of Planetary Motion

3) Newton’s Universal Law of Gravitation f = GMm/R

^{2 }
4) Lorentz’s
Effects

**Hammers Fall Faster Than Feathers**

After all, among other things,
the hammer does indeed ‘fall’ faster than the feather. Try it on a small
asteroid.

__Conclusion__

It is postulated that criteria
for validity of theories should be as follows:

1) If two theories are equally broad in their
powers of description, the simpler is more valid.

2) If there are
two theories and one has broader powers of description, the broader description
is more valid.

**Star-Bows, the Keys to a Revolution in Views on Mathematical Physics**

**+ X**

**Dr. Robert Duncan-Enzmann, designer of the Enzmann Starship**
physicist, scientist, astronomer, geologist, archaeologist, historian, linguist, medical doctor

British Embassy School, Peking, China; Univ. London; WW II USN, AC; RN, AB Harvard; ScB Hon., London; Standard, MSc, Witwatersrand; Nat Sci Scholar; MIT course work; Royal Inst. Uppsala Swed.; PhD/MD Cuidad Juarez, Mex.; Pacific Radar: Greenland Gap-filler, Canada DEW-line; SAGE; Pacific PRESS; California ATLAS, BMEWS; ICBM; Kwajalein Atoll ICBM intercept; TRADEX; Mars Voyager; Cryptography.

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