In order to understand how an object behaves as it attempts to
leave a massive gravitational body (neuron star, black hole) it is
necessary to work out the form of the formula for escape velocity under
the condition of extreme velocity that such an object would have to travel
in order to have any chance of escaping such a gravitational field.
Since such an extreme velocity would have to be near that of the
speed of light the formula for escape velocity must take into account the
effects of special relativity. Now,
in order to solve for this formula of relativistic escape velocity we must
first look at the classical formula for escape velocity for a
gravitational field,
This
formula comes from the energy formula
where
must
be used. This formula, unlike
the classical formula for kinetic energy, goes to infinity as the velocity
v goes to
the speed of light c.
Now, the other side of the classical formula for escape velocity,
the potential energy, is unchanged under relativistically significant
velocities. This is the case
do to the law of conservation of energy.
If the law of conservation of energy is to be maintained then it is
necessary that the potential energy be the same regardless of the path an
object takes through a gravitational field.
If the energy a gravitational field imparted to an object were to
increase or decrease as a result of an object travelling through the field
at near the speed of light then it would be possible to send an object
into a gravitational field at non-relativistically significant velocity
and then send the object out at relativistically significant velocity.
In this way, by the two paths, the low velocity inbound path and
the high velocity outbound path, having different potential energies,
energy could be created or destroyed simply by sending particles around
such a path, thereby breaking the law of conservation of energy.
So, replacing the classical kinetic energy formula with the
relativistic kinetic energy formula within the classical formula for
evaluating escape velocity gives the relativistic formula
Unlike
the classical formula, both sides of this equation are capable of reaching
infinite energy. Reordering in terms of velocity gives
When
we take
For
this formula, as the mass of the gravitational body approaches infinity,
and/or an objects proximity to the body approaches zero the escape
velocity approaches c,
the speed of light. However,
for black hole theory to be valid the escape velocity must exceed the
speed of light as the mass approaches infinity and/or the distance
approaches zero. Therefore,
relativistic escape velocity proves that no gravitational body can ever
reach sufficient mass to form a black hole.
Now, this result is not unexpected.
Rather it reflects the dissymmetry of the idea of black holes, the
idea of a gravitational body existing into which an object could enter but
not escape. By symmetry, any
path by which an object enters a gravitational field, if reversed, is a
path by which the object could exit that field.
And so, if a gravitational body existed that would require more
than an infinite amount of energy to escape then that body would impart an
equal, greater than infinity energy on any object entering that body.
As such, since such a gravitational body would require greater than
an infinity of energy to escape, since escaping it would require more than
an infinity of energy it would impart more than an infinity of energy to
any object that was to enter its field and so would give any such object
the energy to escape its field. And
so, in order for a gravitational body to exist from which nothing could
escape, that body would have to impart less energy to objects entering its
field than it draws from objects that attempt to leave its field.
If gravitational fields were to behave in this way then energy
could be created from nothing and the law of conservation of energy would
be invalid. Since the law of
conservation of energy is valid, black holes are not. |