《时间简史―从大爆炸到黑洞》 ――史蒂芬?霍金

A Brief History of Time - Stephen Hawking... Chapter 2
standard of rest. One could equally well say that body A was at rest and body B was moving at constant speed
with respect to body A, or that body B was at rest and body A was moving. For example, if one sets aside for a
moment the rotation of the earth and its orbit round the sun, one could say that the earth was at rest and that a
train on it was traveling north at ninety miles per hour or that the train was at rest and the earth was moving
south at ninety miles per hour. If one carried out experiments with moving bodies on the train, all Newton’s laws
would still hold. For instance, playing Ping-Pong on the train, one would find that the ball obeyed Newton’s laws
just like a ball on a table by the track. So there is no way to tell whether it is the train or the earth that is moving.
The lack of an absolute standard of rest meant that one could not determine whether two events that took place
at different times occurred in the same position in space. For example, suppose our Ping-Pong ball on the train
bounces straight up and down, hitting the table twice on the same spot one second apart. To someone on the
track, the two bounces would seem to take place about forty meters apart, because the train would have
traveled that far down the track between the bounces. The nonexistence of absolute rest therefore meant that
one could not give an event an absolute position in space, as Aristotle had believed. The positions of events
and the distances between them would be different for a person on the train and one on the track, and there
would be no reason to prefer one person’s position to the other’s.
Newton was very worried by this lack of absolute position, or absolute space, as it was called, because it did
not accord with his idea of an absolute God. In fact, he refused to accept lack of absolute space, even though it
was implied by his laws. He was severely criticized for this irrational belief by many people, most notably by
Bishop Berkeley, a philosopher who believed that all material objects and space and time are an illusion. When
the famous Dr. Johnson was told of Berkeley’s opinion, he cried, “I refute it thus!” and stubbed his toe on a
large stone.
Both Aristotle and Newton believed in absolute time. That is, they believed that one could unambiguously
measure the interval of time between two events, and that this time would be the same whoever measured it,
provided they used a good clock. Time was completely separate from and independent of space. This is what
most people would take to be the commonsense view. However, we have had to change our ideas about space
and time. Although our apparently commonsense notions work well when dealing with things like apples, or
planets that travel comparatively slowly, they don’t work at all for things moving at or near the speed of light.
The fact that light travels at a finite, but very high, speed was first discovered in 1676 by the Danish astronomer

The fact that light travels at a finite, but very high, speed was first discovered in 1676 by the Danish astronomer
Ole Christensen Roemer. He observed that the times at which the moons of Jupiter appeared to pass behind
Jupiter were not evenly spaced, as one would expect if the moons went round Jupiter at a constant rate. As the
earth and Jupiter orbit around the sun, the distance between them varies. Roemer noticed that eclipses of
Jupiter’s moons appeared later the farther we were from Jupiter. He argued that this was because the light from
the moons took longer to reach us when we were farther away. His measurements of the variations in the
distance of the earth from Jupiter were, however, not very accurate, and so his value for the speed of light was
140,000 miles per second, compared to the modern value of 186,000 miles per second. Nevertheless,
Roemer’s achievement, in not only proving that light travels at a finite speed, but also in measuring that speed,
was remarkable

A Brief History of Time - Stephen Hawking... Chapter 2
coming toward them at different speeds, but light's speed relative to the ether would remain fixed. In particular,
as the earth was moving through the ether on its orbit round the sun, the speed of light measured in the
direction of the earth's motion through the ether (when we were moving toward the source of the light) should
be higher than the speed of light at right angles to that motion (when we are not moving toward the source). In
1887Albert Michelson (who later became the first American to receive the Nobel Prize for physics) and Edward
Morley carried out a very careful experiment at the Case School of Applied Science in Cleveland. They
compared the speed of light in the direction of the earth's motion with that at right angles to the earth's motion.
To their great surprise, they found they were exactly the same!
Between 1887 and 1905 there were several attempts, most notably by the Dutch physicist Hendrik Lorentz, to
explain the result of the Michelson-Morley experiment in terms of objects contracting and clocks slowing down
when they moved through the ether. However, in a famous paper in 1905, a hitherto unknown clerk in the
Swiss patent office, Albert Einstein, pointed out that the whole idea of an ether was unnecessary, providing one
was willing to abandon the idea of absolute time. A similar point was made a few weeks later by a leading
French mathematician, Henri Poincare. Einstein’s arguments were closer to physics than those of Poincare,
who regarded this problem as mathematical. Einstein is usually given the credit for the new theory, but
Poincare is remembered by having his name attached to an important part of it.
The fundamental postulate of the theory of relativity, as it was called, was that the laws of science should be
the same for all freely moving observers, no matter what their speed. This was true for Newton’s laws of
motion, but now the idea was extended to include Maxwell’s theory and the speed of light: all observers should
measure the same speed of light, no matter how fast they are moving. This simple idea has some remarkable
consequences. Perhaps the best known are the equivalence of mass and energy, summed up in Einstein’s
famous equation E=mc2 (where E is energy, m is mass, and c is the speed of light), and the law that nothing
may travel faster than the speed of light. Because of the equivalence of energy and mass, the energy which an
object has due to its motion will add to its mass. In other words, it will make it harder to increase its speed. This
effect is only really significant for objects moving at speeds close to the speed of light. For example, at 10
percent of the speed of light an object’s mass is only 0.5 percent more than normal, while at 90 percent of the
speed of light it would be more than twice its normal mass. As an object approaches the speed of light, its mass
rises ever more quickly, so it takes more and more energy to speed it up further. It can in fact never reach the
speed of light, because by then its mass would have become infinite, and by the equivalence of mass and
energy, it would have taken an infinite amount of energy to get it there. For this reason, any normal object is
forever confined by relativity to move at speeds slower than the speed of light. Only light, or other waves that
have no intrinsic mass, can move at the speed of light.

An equally remarkable consequence of relativity is the way it has revolutionized our ideas of space and time. In
Newton’s theory, if a pulse of light is sent from one place to another, different observers would agree on the
time that the journey took (since time is absolute), but will not always agree on how far the light traveled (since
space is not absolute). Since the speed of the light is just the distance it has traveled divided by the time it has
taken, different observers would measure different speeds for the light. In relativity, on the other hand, all
observers must agree on how fast light travels. They still, however, do not agree on the distance the light has
traveled, so they must therefore now also disagree over the time it has taken. (The time taken is the distance
the light has traveled

Figure 2:1
Using this procedure, observers who are moving relative to each other will assign different times and positions
to the same event. No particular observer’s measurements are any more correct than any other observer’s, but
all the measurements are related. Any observer can work out precisely what time and position any other
observer will assign to an event, provided he knows the other observer’s relative velocity.
Nowadays we use just this method to measure distances precisely, because we can measure time more
accurately than length. In effect, the meter is defined to be the distance traveled by light in
0.000000003335640952 second, as measured by a cesium clock. (The reason for that particular number is that
it corresponds to the historical definition of the meter

A Brief History of Time - Stephen Hawking... Chapter 2
terms of time and the speed of light, so it follows automatically that every observer will measure light to have
the same speed (by definition, 1 meter per 0.000000003335640952 second). There is no need to introduce the
idea of an ether, whose presence anyway cannot be detected, as the Michelson-Morley experiment showed.
The theory of relativity does, however, force us to change fundamentally our ideas of space and time. We must
accept that time is not completely separate from and independent of space, but is combined with it to form an
object called space-time.
It is a matter of common experience that one can describe the position of a point in space by three numbers, or
coordinates. For instance, one can say that a point in a room is seven feet from one wall, three feet from
another, and five feet above the floor. Or one could specify that a point was at a certain latitude and longitude
and a certain height above sea level. One is free to use any three suitable coordinates, although they have only
a limited range of validity. One would not specify the position of the moon in terms of miles north and miles
west of Piccadilly Circus and feet above sea level. Instead, one might describe it in terms of distance from the
sun, distance from the plane of the orbits of the planets, and the angle between the line joining the moon to the
sun and the line joining the sun to a nearby star such as Alpha Centauri. Even these coordinates would not be
of much use in describing the position of the sun in our galaxy or the position of our galaxy in the local group of
galaxies. In fact, one may describe the whole universe in terms of a collection of overlapping patches. In each
patch, one can use a different set of three coordinates to specify the position of a point.
An event is something that happens at a particular point in space and at a particular time. So one can specify it
by four numbers or coordinates. Again, the choice of coordinates is arbitrary; one can use any three
well-defined spatial coordinates and any measure of time. In relativity, there is no real distinction between the
space and time coordinates, just as there is no real difference between any two space coordinates. One could
choose a new set of coordinates in which, say, the first space coordinate was a combination of the old first and
second space coordinates. For instance, instead of measuring the position of a point on the earth in miles north
of Piccadilly and miles west of Piccadilly, one could use miles northeast of Piccadilly, and miles north-west of
Piccadilly. Similarly, in relativity, one could use a new time coordinate that was the old time (in seconds) plus
the distance (in light-seconds) north of Piccadilly.

It is often helpful to think of the four coordinates of an event as specifying its position in a four-dimensional
space called space-time. It is impossible to imagine a four-dimensional space. I personally find it hard enough
to visualize three-dimensional space! However, it is easy to draw diagrams of two-dimensional spaces, such as
the surface of the earth. (The surface of the earth is two-dimensional because the position of a point can be
specified by two coordinates, latitude and longitude.) I shall generally use diagrams in which time increases
upward and one of the spatial dimensions is shown horizontally. The other two spatial dimensions are ignored
or, sometimes, one of them is indicated by perspective. (These are called space-time diagrams, like Figure
2:1.)

Figure 2:2
For example, in Figure 2:2 time is measured upward in years and the distance along the line from the sun to
Alpha Centauri is measured horizontally in miles. The paths of the sun and of Alpha Centauri through
space-time are shown as the vertical lines on the left and right of the diagram. A ray of light from the sun
follows the diagonal line, and takes four years to get from the sun to Alpha Centauri.
As we have seen, Maxwell’s equations predicted that the speed of light should be the same whatever the
speed of the source, and this has been confirmed by accurate measurements. It follows from this that if a pulse
of light is emitted at a particular time at a particular point in space, then as time goes on it will spread out as a
sphere of light whose size and position are independent of the speed of the source. After one millionth of a
second the light will have spread out to form a sphere with a radius of 300 meters; after two millionths of a
second, the radius will be 600 meters; and so on. It will be like the ripples that spread out on the surface of a
pond when a stone is thrown in. The ripples spread out as a circle that gets bigger as time goes on. If one
stacks snapshots of the ripples at different times one above the other, the expanding circle of ripples will mark
out a cone whose tip is at the place and time at which the stone hit the water Figure 2:3.

A Brief History of Time - Stephen Hawking... Chapter 2
Figure 2:3
Similarly, the light spreading out from an event forms a (three-dimensional) cone in (the four-dimensional)
space-time. This cone is called the future light cone of the event. In the same way we can draw another cone,
called the past light cone, which is the set of events from which a pulse of light is able to reach the given event
Figure 2:4.

Figure 2:4
Given an event P, one can divide the other events in the universe into three classes. Those events that can be
reached from the event P by a particle or wave traveling at or below the speed of light are said to be in the
future of P. They will lie within or on the expanding sphere of light emitted from the event P. Thus they will lie
within or on the future light cone of P in the space-time diagram. Only events in the future of P can be affected
by what happens at P because nothing can travel faster than light.
Similarly, the past of P can be defined as the set of all events from which it is possible to reach the event P
traveling at or below the speed of light. It is thus the set of events that can affect what happens at P. The
events that do not lie in the future or past of P are said to lie in the elsewhere of P Figure 2:5.