When we consider the experiment of Fizeau in the light of a vacuum containing dragged ether
the following physics should be expected. The ether in the water molecules is most
under influence by the Oxygen en Hydrogen atoms. Although the Moon and Sun have
gravity influences these effects are small compared to the effects of the
magnetic- and electric fields in the water molecules.
When the water moves in Fizeau’s
experiment the ether between the water molecules is dragged by the water. Light
travels through the moving water as if the water were at rest. For the observer
at rest with the water it is not the water that moves but the laboratory of Fizeau.
This is also the case for light traveling
through the water when dragged ether is assumed. The speed of light in water is
c/n: the speed of
light divided by index of water. The light in the water has no conception of
the movement of the water. The ether moves through the water as if the water
stand still and the laboratory were moving. The ether is under the influence of
the water and therefore moves like the water. The light has no idea whether it
moves against or with the current. Only for the observer outside the water in rest
with the laboratory there is movement of water.
Assuming the presence of dragged ether, light
traveling in the direction of the water has a distance to overcome L
minus the distance the water is traveling during this time. And reversed,
against the direction of the water, the path through the water is comparably
longer.
Calculating the theoretical drag in this way
one calculates a “drag” of:
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The theoretical shift in interference lines is
calculated at d=0.23; exact the value
measured by Fizeau. The experiment of Fizeau matches perfectly with the theoretical assumption of
dragged ether.
The dimensions of the Fizeau
experiment are:
L=1.5 m v=7 m/sec l=5.310^-7
m n=1.33
c=299792458
m/sec
With L the length, n the index
for water, l the wavelength of the light, v the current speed, f the
drag factor of Fresnel and c the speed of light. The calculated time
difference with Fresnel’s drag factor is:
![]()
Because
we find
approximately:
![]()
The optical difference in interference lines
is:
![]()
According to Fresnel’s theory the drag factor
is f=0.435 and therefore the theoretical shift lines has to be d=0.203.
The measured values by Fizeau
are: f=0.48 d=0.23
The difference between the theoretical and the
measured value is 10%.
When we determine the theoretical values
according to the existence of dragged ether, the path decreases/increases in
accordance with the distance the water is flowing during the time the light
travels through the water. We derive the equations:
![]()
The first formula t1 gives the time the
light needs to travel through the water with the current. The time needed for
going against the flow is given by formula t2. The theoretical
difference in interference lines is then calculated at:
d=0.23
The theoretical shift with dragged ether and
the experiment of Fizeau is a perfect match with the
measured values. The experiment of Fizeau becomes therefore strong empirical evidence for
dragged ether.
Next Chapter Questions or remarks?