Derivation
of the photon coordinate path equation.
Start
with the radial only Schwarzschild metric.

For
a photon the proper time dS is zero and the coordinate
velocity dr/dt of a photon is easily solved to give:

The
above equation then needs to be integrated to obtain a result in terms of r and
t. This is most easily achieved by inverting the equation to obtain dt/dr and then integrating with respect to r to obtain:
![\int_{r_1}^{r_2}\left(\frac{dt}{dr}\right){dr}=\int_{r_1}^{r_2}c \left( 1-\frac{2m}{rc^2}\right)^{-1} {dr} = \left[(rc^2+2m \,\,ln(2m-rc^2))/c^3\right]_{r_1}^{r_2}](LightDerivation_files/image003.gif)
Inserting
the values r1 and r2 for r gives:

The
log of a negative number is imaginary and the reader should satisfy themselves
that a real solution is only obtained when r1 and r2 are both greater than 2m
or both are less than 2m. Therefore there is no continuous path across the
event horizon for a photon. A photon can approach the event horizon from above
or below but it can not cross it.
Most
text books get around this problem by inserting an absolute function inside the
log function to force the result to be real and prove that the photon crosses
the event horizon. There is no mathematical justification for that and in fact
it is mathematically and intellectually unethical and unscientific to do that.
You can not change the rules of maths to give the result that you are biased
towards.
Derivation
of the particle coordinate path equation.
The
derivation of the particle path is somewhat more involved and the reader is
referred to the mathpages
derivation by Kevin Brown. As far as I can tell the derivation is correct
except that Kevin Brown succumbs to the usual temptation to insert an ad-hoc
absolute function so that the result agree with the accepted traditional
physical interpretation rather than let the maths speak for itself and question
the accepted physical interpretation. These are the final corrected steps shown
below.
Starting
with:
![t = \sqrt{{R \over 2m} -1}\left[\left( {R \over 2} +2m \right)\alpha + \left(R \over 2\right) sin(\alpha)}\right] - 4m\sqrt{-1}\,\,arctan\left(cos(\alpha)-1 \over sin(\alpha)\sqrt{1-R/2m} \right)](LightDerivation_files/image005.gif)
Substituting
the equation
becomes:
![]()
Substituting
the identity
we get
![]()
Now
the final substitution of
gives:
![]()
and not
![]()
as
claimed by Kevin Brown. When I first pointed this out to K. Brown he removed
the ad-hoc absolute function in the last term, but unfortunately he put it back
in again later when he realised it did not agree with the accepted physical
interpretation.
The
alpha variable that appears in the particle equation is a parametric variable.
It can be removed to give a normal Cartesian equation by noting that mathpages
gives the radial part of the proper motion of a particle as r=R(1+cos(alpha))/2 which is easily solved to give alpha =
acos(2r/R-1) which is the form used in the applets. Later it is shown that
using the Cartesian version offers valuable insight into the nature of time
itself that is obscured by using the parametric equations.
Update
Since
I posted the above comments about the mathpages derivation, Kevin Brown has
updated his page to try and justify the insertion of the absolute function into
the equation. His argument is basically that the equation is discontinuous
across the event horizon and therefore the constant of integration is allowed
to be different above and below the event horizon. His argument is correct to a
point but fails in its application. Below the event horizon the logarithmic
term on the end has a negative argument and becomes imaginary making the
solution for t a complex value and below the event horizon the equation has
this form:
![]()
At
this point Kevin Brown chooses to add a constant of integration of (-i*pi) and to interpret the coordinate time of the motion in
terms of only the real part of the complex equation. He is free to do that, but
when the apogee is below the event horizon (R < 2m) the coordinate motion is in total
contradiction to the motion in proper time. The former shows the particle
falling to the event horizon and all time values for r<R have no real part,
while the latter shows the particle falling to the central singularity ad all
proper time values for r>R have no real part. By choosing to add a constant
of (-i*pi) Kevin Brown (and most text books) is
choosing to accept a singularity of infinite mass density as a physically real
and he is also choosing to accept that light travels backwards in time below
the event horizon.
On
the other hand, I am free to choose not
to add a constant of integration and by doing so, the contradiction of
coordinate motion and proper motion is removed, the central singularity of
infinite density is removed and we are not required to accept that light
travels backwards in time below the event horizon. In other words all the
paradoxes of the conventional interpretation are not an inevitable conclusion
of General Relativity. I have shown that there is an equally mathematically
valid interpretation that removes all the contradictions and paradoxes.
It
seems Kevin Brown has not investigated the implications of setting the apogee
to values of (R <2m) in his own equations as I have. I am sure that if he
does, he will find it a revelation.
Kevin Brown is clearly a very intelligent person and very knowledgeable
in geometry, calculus and General Relativity (I suspect he is a professor) and
I would love for him to investigate my claims stated in this website with an
open mind. I have known for a long time that ‘something’ is wrong with the
conventional interpretation of black holes, but I would not have been able to
demonstrate that mathematically without the equations derived by Kevin Brown.
In that sense Kevin Brown deserves 90% of the credit for my work here and we
differ only in the final physical interpretation of the equations.
I
have no direct contact with Kevin Brown, but he has been updating his website
in response to my questions and objections here and elsewhere on the internet.
The evolution of his webpage (Radial paths in a Spherically Symmetric Field) is
documented in this list with approximate dates. (Sometimes it is a couple of
days before I notice the webpage has changed).
Radial
paths in a Spherically Symmetric Field 6thOct2008
Radial
paths in a Spherically Symmetric Field 21stNov2008
Radial
paths in a Spherically Symmetric Field 23rdNov2008
Radial
paths in a Spherically Symmetric Field 27thNov2008
Radial
paths in a Spherically Symmetric Field 20thDec2008
Until
further notice I can be contacted at my physicsforums blog here
or at the email address given in the introduction.
Please
do not post questions about this website in the public part of the
physicsforums, as posting anything relating to a website that questions the
mainstream view can earn you an instant ban. Even posting something like “I
don’t think this website is right” and posting a link to this website can get
you banned. You have been warned.
©
2008 KevPegrume