space engine

1. Space Engine
Benjamin Yiwen Faerber
January 16, 2017
K is thermal conductivity, A is surface area dQ/dt is the power transfer, and dT/dx is
the temperature gradient across the pipe.
dQ
dt
= KA
dT
dr
(1)
Reference https://www.physicsforums.com/threads/change-in-temperature-of-water-as-
it-flows-through-a-pipe.450206/
r
r−x
1
r
dr =
Ts
Tw
k2πl
P
dT (2)
ln
r
r − x
=
k2πl
P
(TS − TW ) (3)
With the movement of water particles the temperature changes. This is a general
indication that water is a magic fluid! The movement of a water particle through a tube
is comparable to the movement of a train on the rail. For the movement of the train the
laws of special theory of relativity are applicable. Therefore the laws of movement must be
combined with temperature, maybe also with the laws of special theory of relativity. The
theory of special relativity theory can be easily understood, when one sits on a train. One
is then in a moving inertial system which moves relative to the stationary inertial system,
which is the outside environment, and one distinguishes himself through the velocity. The
special relativity theory postulates to draw a linear slope or a straight line in a coordinate
system, which represents the moving inertial system. Alternatively the straight line draws
an angle to the x-axis of the static coordinate system. Actually a very simple theory, which
is not complete, as the speed of light cannot be the maximum velocity. Instead one has
to combine the special theory of relativity with the temperature of a quantum mechanical
system.
1. v (velocity) must be connected to T (Temperature).
2. v is infinite
3. An inertial system which moves on a geodesic, moves above a vacuum, and this vacuum
must be put into relation to the movement of the inertial system.
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2. The von-Neumann type interaction
n
cn|φn |Φ0 →
n
|φn |Φn (4)
may be described by the Hamiltonian
H = γ
n
α|φn φn|ˆp (5)
The Hamiltonian should describe an open boundary quantum system. The wave function
of the pointer after time t is
Φn (x, t) = Φ (x − γαnt) (6)
A measurement is ’complete’ when the wave packets Φn for different n are approximately
orthogonal (and therefore equal to the Schmidt states Φn (t).
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