HPS 0410 | Einstein for Everyone |

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John D. Norton

Department of History and Philosophy of Science

University of Pittsburgh

- Why We Need a Better Diagram for Visualizing Black Holes: Conformal Diagrams
- An Analogy to Perspective Drawings
- A Conformal Diagram of a Minkowski Spacetime
- A Conformal Diagram of a Black Hole formed from Collapsing Matter
- Conformal Diagram of a Fully Extended, Schwarzschild Black Hole
- Einstein-Rosen Bridges
- More...
- What You Should Know

The spacetime diagram we used so far for visualizing black holes is not a very good representation of a black hole. It cannot represent the continuous spacetime trajectory of a body falling in as a continuous curve. There is no point in it at which the body is at an event on the event horizon. It does not even show all the structures present in a black hole. There are other parts to spacetime we do not see on it.

The diagram also breaks with our familiar slogan "time goes up--space goes across." Inside the event horizon for this figure, time goes across in the sense that horizontal lines pointing towards the singularity are future directed timelike curves.

There is a better way of representing the black hole. It is to use a conformal diagram that brings in infinities and represents them as points on the diagram. These diagrams will include purely fictitious points like the end points of the timelike worldlines of objects that persist for infinite time. There is no such end point, but they will be on the diagram and prove very useful to us.

At first the idea of a diagram that represents such fictitious points at infinity might seem a little mysterious. But the idea is actually quite familiar in another context, that of perspective drawing. Imagine an infinite, two dimensional Euclidean plane criss-crossed by a grid of lines. An ordinary drawing, looking straight down from overhead, cannot capture more than a small portion of the plane.

We know some of properties of the grid. All the
north-south lines are parallel and never meet. They just go off to a
north and a south infinity. Sometimes we say that these parallel lines
"meet" at infinity. The talk suggests a
kind of Valhalla for valiant, but departed lines where they all finally
meet to celebrate battles lost and won.
Of course we don't intend that "meet at
infinity" talk to be taken literally. |

The north-south lines are crossed by east-west lines. An analogous story can be told for them.
They are parallel and "meet" at a *different* infinity. This "meet at
infinity" talk is just a way of reifying the different directions in which two
sets of lines persist in moving.

Now imagine that we move our gaze towards the horizon from our overhead position. We can now see an infinite portion of the plane. If we make a drawing of what we see, we can see the entire length of infinite lines, or at least one half of them extending infinitely. |

In this new perspective drawing, we can actually see the points at infinity at which the parallel lines meet. These points at infinity lie on the horizon. All the north-south lines meet at one point on the horizon. It is the North vanishing point, but let us call it the "north-infinity." All the east-west lines meet at a different point on the horizon. It is the East vanishing point, but let us call it the "east infinity."

Of course no one thinks these points represent a real place on the plane. The fact that a line in the figure actually connects to the north-infinity point just encodes the fact that the line really keeps going north indefinitely. Analogously, the fact that a line in the figure connects to a different point at infinity, the east-infinity, just encodes the fact that the line really keeps going indefinitely in a different direction, east. In short, the point on the horizon is a fictitious point that represents the infinity never actually reached by the lines.

A traditional perspective drawing does not show us the full, infinite plane. For that, we need an even more distorted image, an overhead view such as produced by a camera with a "fisheye" lens. | The horizon in all directions in visible in this fisheye image of a mountaintop. http://en.wikipedia.org/wiki/File:Mountaintop_fisheye.jpg |

Fisheye image shows all four walls of the banquet hall in Hellbrunn Palace, Salzburg.

http://en.wikipedia.org/wiki/File:Hellbrunn_banqueting_hall_ceiling_fisheye_projection.jpg

Finally perspective drawings must pay a price for being able to show the infinite length of a line. In the overhead view, a drawing can be scaled properly. That means that one inch on the drawing can always correspond to one mile in the real plane. This cannot be done in a perspective drawing. A length of one inch in one part of the perspective drawing might correspond to one mile in the real plane. But one inch in a part of the drawing close to the points at infinity might represent a much greater--even infinite--distance in the real plane.

Just like the overhead view of the North-South and East-West lines, the spacetime diagrams we have used so far for a Minkowski spacetime only show a small portion of the spacetime. We can also have a diagram in which the points at infinity become visible. We used a perspective transformation before. This time we shall use a "conformal" transformation to produce a "conformal diagram." | A conformal transformation has the property of leaving lightlike curves unaffected, but stretching and shrinking times and spatial distances. We need not pursue the messy details here. |

Recall that a timelike geodesic is just a point moving inertially and a spacelike geodesic is just the familiar straight line of ordinary geometry. A lightlike or null geodesic is the curve traced by a light pulse moving freely. | A Minkowski spacetime has many different sorts of infinities. They come from the types of curves in the spacetime. It has timelike, space and lightlike geodesics. Each has their own infinity. Note as before that these infinities in the diagram are fictitious points. There is no point in spacetime corresponding to them, just as there is no point in space corresponding to the vanishing point of a perspective drawing. |

First, here is the conformal
diagram of a Minkowski spacetime. This is the complete
spacetime. It includes all of the infinity of space and the infinity of
time through which things persist.
This diagram gives the simplest case in which we consider just one dimension of space. Note the three types of infinities: timelike, lightlike and spacelike. They correspond to the different vanishing points in an ordinary perspective drawing. Let us investigate each in turn. |

Here is an ordinary Minkowski spacetime with the timelike geodsics that stretch from the infinite past to the infinite future. The diagram can only show a finite portion of each geodesic. |

Here are the same timelike
geodesics shown on the conformal diagram. We can now see them in
their entirety, stretching from past timelike infinity i^{-} to
future timelike infinity i^{+}.
It is important to note that the distances along the curves do not represent properly scaled times elapsed. 1/4"
length of the timelike geodesic in the middle of the curve might
represent a day of elapsed time. The final 1/4", at the end of the
geodesic where it joins i Note that we can only be assured that
timelike geodesics--corresponding to unaccelerated motions--will
stretch from past timelike infinity i |

Here are lightlike geodesics on a spacetime diagram. they stretch from the infinite past to the infinite future. Only a small portion of each full curve can be shown. |

Here are the same lightlike
geodesics displayed in their entirety on a conformal diagram.
They extend from past lightlike infinity to future lightlike infinity.
Note that these infinities are not just points, but a complete line,
rather like the line of the horizon in a perspective drawing.
These infinities are sometimes called "null" infinity and lightlike curves, "null" curves, since the time elapsed along a lightlike curve is zero, that is, "null." The symbol for lightlike infinity is a script i, which looks like . To some people this looks like a curly J. Since a script i is hard to render in html, it is often called "scri." |

Finally, a Minkowski spacetime is populated with
spacelike curves as well. They form the
spacelike hypersurfaces that are the "nows" of the spacetime.
They extend from infinity to infinity and only a small portion of each surface can be shown. |

Here are spacelike
curves taken from these spatial hypersurfaces. They are shown in
their entirety and stretch from one spacelike infinity i^{0} to
another spacelike infinity i^{0}.
Distances in the figure no longer correspond to properly scaled
distances in space. 1/4" at the center of figure on one of these curves
may correspond to a mile; the last 1/4" of the curves, where they
connect to i |

That light travels at the same velocity c is encoded
into the diagrams by the particular fact that all lightlike geodesics
are oriented at 45^{o} to the
vertical. This important geometric fact is shown in the
figure. |

That timelike geodesics represent points moving at
less that the speed of light has a similar geometric expression.
Such curves are, at every event, pointed in a direction that makes
an angle of less that 45 Since timelike geodesics generally change their direction from event to event in a conformal diagram, we need to be a little clearer about what this means. It means this. Take any event on the worldline, such as shown in the figure. Bring a straight edge to the event so that the straight edge is tangent to the curve at that event. Then that straight edge must make an angle of less than
45 This must be true of every event on the timelike geodesic. |

The important properties of a
conformal diagram are threefold:

--Time once again always goes up in the figure; and space goes across.

--Lightlike curves are always at 45^{o}. The light cones no longer tip
over in the figure. Timelike curves are always directed at less than
45^{o} with the vertical; and spacelike curves are always at greater
than 45^{o} with vertical.

--The same intervals on the figure no longer correspond to the same times
elapsed and spaces covered. An interval of say one inch on a timelike curve in
the middle of the diagram might correspond to one day of elapsed time. The last
inch of the timelike curve terminating in i^{+} corresponds to an
infinite time elapsed.

It is not at all obvious that we have gained anything with the conformal diagram of a Minkowski spacetime; we just seem to be saying what we already knew in a new, unfamiliar way. In the case of a black hole, however, the conformal diagram makes it easy to see properties of the spacetime that were formerly quite hard to see.

Here is the conformal diagram of a black hole that has been produced by collapsing matter. This is a black hole of the simplest type, one associated with a Schwarzschild spacetime. This black hole has no electric charge and no angular momentum (i.e. it isn't spinning). You'll see immediately how unrealistic that is. Any collapsing cloud of matter is likely to have a very complicated structure and certainly not be so perfectly symmetric that it collapses without turning. However the simplicity makes it easy for us to see its properties.

To read the diagram,
start at the bottom. The worldlines of collapsing matter come out of
past timelike infinity, i^{-}. As they proceed upward through
time, they collapse onto themselves.
They have formed a black hole when collapsed sufficiently to
generate an event horizon, which is indicated as the line at
45 The novelty is that the spacetime is now divided into two regions, marked I and II. Region I is an ordinary spacetime--in fact the familiar Schwarzschild spacetime we've spent so much time looking at. It has the familiar timelike, lightlike and spacelike infinities. The region II is the region inside the black hole, past the event horizon. |

Let us now add the worldlines of a planet and a traveler that leaves the planet and
falls into the black hole.
The planet's worldline originates in past timelike infinity,
i The traveler leaves the planet and passes from region I into the black hole region II and into the singularity. |

The event horizon marks
the boundary of no return. We can see that by recalling that a traveler
must alway travel at less than the speed of light. That is, the
traveler's worldline must always be at less that 45^{o} to the
vertical.
That means that the traveler can always pull away from the black hole, as long as the event horizon has not been passed. If the traveler strays close to event horizon at A, or closer at A',
or even closer at A'', it is evident from the geometry of the figure
that the traveler can always find a trajectory that will end in future
timelike infinity. For the event horizon itself marks the boundary of a
curve 45 Once the event horizon is passed--say the traveler is at event B--it
is too late. All trajectories at less than 45 Take a moment; stare at the figure; and convince yourself that all
this is correct. Remember the key fact: the traveler's worldline must
everywhere make an angle of less than 45 |

Finally we can use the conformal diagram to trace
the signals sent by the traveler back to
the planet.
The diagram shows the traveler sending out light signals, which
propagate along the 45 The diagram shows that only light signals emitted before the traveler passes the event horizon will make it to the planet. Once the traveler has passed the event horizon, all the light signals will end up in the singularity. Turning it around, if a planet observer waits and watches the while the traveler falls in, the rate of signals received will slow down. The planet observer would need to live for all eternity of time to intercept all the signals sent out by the traveler before the traveler reaches the event horizon. |

The black hole formed by collapsing matter is the simplest black hole. It is far from the most interesting. By solving Einstein's field equations--that is by consulting his book of universes--we find a closely related black hole. It is like the one we've just seen, but was not formed by collapsing matter. It has existed for all time. It is known as the "fully extended, Schwarzschild black hole."

We can construct one mathematically by starting with just the matter free part of the Schwarzschild spacetime. We then extend that piece of spacetime with more matter free spacetime by means of Einstein's gravitational field equations. If we keep extending the spacetime in that way, we end up with a new and interesting black hole. Here is a conformal diagram of it. | Recall the jigsaw puzzle analogy. The extension is like adding more pieces to an incomplete jigsaw puzzle. |

The great novelty of the new black hole is that it is twice the size of the old one. On the "other side" of the event horizon is a complete duplicate of the exterior of the black hole, the region III. Just as region I is an infinite space surrounding the black hole, region III is another infinite space just like it.

Everything that happens in region I can happen in region III. Both can have planets and moons and space travelers. In region I we can have a planet that passes from past timelike infinity to future timelike infinity and sends out a traveler who falls into the black hole. And we have the same thing for region III: a planet that passes from past timelike infinity to future timelike infinity and sends out a traveler who falls into the black hole.

The second duplication is equally striking. The counterpart of the singularity in the future is a new singularity in the past. It is surrounded by a region that duplicates region II, the inside of the black hole. This new singularity/region IV behaves like the reverse of the future singularity. Just as things fall into the future singularity, things fall out of the past singularity and into the spacetime. For this reason, the structure is called a "white hole." The diagram shows timelike worldlines of things that are ejected by the past singularity into the regular spacetime regions I and III.

What can come out of the singularity? Ejection from it is the reverse process in time of falling into the future singularity. So anything that can fall into the future singularity can be ejected from the past singularity. That means anything--dinosauars; the socks you lost; TVs showing re-runs of "I love Lucy"; and so on. You might expect that the theory would say that ejecting odd things like that is vastly improbable. The awkward thing is that the theory assigns no probabilities to these possibilities. It just says that this is possible and that is impossible. Ejecting dinosaurs is as possible as ejecting the chaotic gush of hot particles and radiation that seems most natural.

The past singularity is a "naked singularity." That means it is not hidden behind an event horizon, like the future singularity, and things that come out of it can reach us. | Before you dismiss the dinosaurs and TVs as crazy, recall that we have one clear example of the existence of a naked singularity. That is the big bang of cosmology. That singularity certainly did eventually eject dinosaurs and TVs, although it did take a while for them to form from the material ejected! There's no news on your socks, however. Did you look behind the drier? |

What about traveling from region I to
the other world of region III? The idea is hugely appealing (if we set
aside worries about tidal forces). We would throw ourselves into a black hole,
which would then prove to be the portal to another world! Alas, it is clear
from the conformal diagram that passing over into the other world is prohibited
to beings like us who cannot travel faster than light. Here is a worldline of a
traveler who makes the passage. You'll see that it is inevitable that, at some
point, the curve must make an angle of more than 45^{o} with the
vertical. That is, the traveler must at some point exceed the speed of light.
Any attempt by travelers who cannot do this would result in a one-way trip into
the singularity.

Proceeding in this way, the conformal diagram enables us to recover lots of information about the fully extended black hole. Is it possible for beings from region I and III to meet somewhere? Yes, in region II. If a traveler falls from a planet into the black hole, how much of the planet's worldline will be visible through light signals to the traveler in the brief moments that remain before the traveler meets the future singularity? Depending on how the traveler falls, an arbitrarily large amount will be visible.

The diagrams shown above are limited in one aspect. A three dimensional space has two of its dimensions suppressed. The space appears merely as a single line, a one dimensional space, marked below as a "spatial hypersurface."

If we restore the two missing dimensions, each point on the hypersurface is really a two dimensional sphere of space enclosing the black hole. As we proceed from one side to the other, the enclosing spheres get smaller and smaller. However, since the geometry is not Euclidean, the spheres do not lose area as fast as you'd expect when we move to spheres successively closer to the singularity. We already saw this effect in the Schwarzschild spacetime of massive bodies like the sun. In this case, however, the effect is stronger. The spheres reach a minimum size and then expand.

The effect can be seen in an embedding diagram in which we show only two of the three dimensions of the spheres. The spheres are now represented by circles. The circles become smaller as we proceed from region I to III. However once they reach a minimum size, they begin to expand. The diagram is very suggestive. It has been called an Einstein-Rosen bridge that connects the two worlds of regions I and III. In a sense it is bridge, but it is only one that travelers who can go faster than light can cross. | The figure below of the Einstein-Rosen bridge is an extension of the familar embedding diagram of the space around the sun, in which the space appears to be stretched like a rubber membrane. |

This short introduction does not even begin to exhaust all the novel and interesting ideas associated with black holes. We have looked only at the simplest case. If we allow that the black hole can have some angular momentum (i.e. it spins) and that it can carry charge, the associated conformal diagram become very much more complicated. Many new regions corresponding to new worlds appear. It does turn out to be possible for us to visit them, if we fall into a black hole and somehow survive the pummeling of tidal forces.

It also turns out that the types of black holes are limited by the factors just mentioned. Once the mass, charge and angular momentum of a black hole are fixed, then all its properties are also determined. That gravitational collapse will always produce a black hole has also been demonstrated in theorems akin to those that demonstrate the inevitability of a big bang singularity. And it has been suggested that when gravitational collapse produces a singularity, that singularity is always hidden behind an event horizon--this is known as "cosmic censorship."

Yet further complications arise if we allow for the quantum nature of matter. It turns out that black holes, especially small ones, become unstable, emit particles and can evaporate!

- How to read conformal diagrams for Minkowski spacetime.
- How to read conformal diagrams for a Schwarzschild black hole.
- How to use those conformal diagrams to determine what happens to travelers and signals exploring the spacetime.