The non-mathematician is seized by a mysterious shuddering1 when he hears of “four-dimensional” things, by a feeling not unlike that awakened2 by thoughts of the occult. And yet there is no more common-place statement than that the world in which we live is a four-dimensional space-time continuum.
Space is a three-dimensional continuum. By this we mean that it is possible to describe the position of a point (at rest) by means of three numbers (co-ordinates) x comma y comma z, and that there is an indefinite number of points in the neighbourhood of this one, the position of which can be described by co-ordinates such as x 1 comma y 1 comma z 1, which may be as near as we choose to the respective values of the co-ordinates x comma y comma z, of the first point. In virtue3 of the latter property we speak of a “continuum,” and owing to the fact that there are three co-ordinates we speak of it as being “three-dimensional.”
Similarly, the world of physical phenomena4 which was briefly5 called “world” by Minkowski is naturally four dimensional in the space-time sense. For it is composed of individual events, each of which is described by four numbers, namely, three space co-ordinates x comma y comma z, and a time co-ordinate, the time value t. The “world” is in this sense also a continuum; for to every event there are as many “neighbouring” events (realised or at least thinkable) as we care to choose, the co-ordinates x 1 comma y 1 comma z 1 comma t 1 of which differ by an indefinitely small amount from those of the event x comma y comma z comma t originally considered. That we have not been accustomed to regard the world in this sense as a four-dimensional continuum is due to the fact that in physics, before the advent6 of the theory of relativity, time played a different and more independent role, as compared with the space coordinates7. It is for this reason that we have been in the habit of treating time as an independent continuum. As a matter of fact, according to classical mechanics, time is absolute, i.e. it is independent of the position and the condition of motion of the system of co-ordinates. We see this expressed in the last equation of the Galileian transformation8 (t prime equals t)
The four-dimensional mode of consideration of the “world” is natural on the theory of relativity, since according to this theory time is robbed of its independence. This is shown by the fourth equation of the Lorentz transformation:
t prime equals StartStartFraction t minus StartFraction v Over c squared EndFraction x OverOver StartRoot 1 minus StartFraction v squared Over c squared EndFraction EndRoot EndEndFraction period
Moreover, according to this equation the time difference normal upper Delta9 t prime of two events with respect to K′ does not in general vanish, even when the time difference normal upper Delta t prime of the same events with reference to K vanishes. Pure “space-distance” of two events with respect to K results in “time-distance” of the same events with respect to K′. But the discovery of Minkowski, which was of importance for the formal development of the theory of relativity, does not lie here. It is to be found rather in the fact of his recognition that the four-dimensional space-time continuum of the theory of relativity, in its most essential formal properties, shows a pronounced relationship to the three-dimensional continuum of Euclidean geometrical space.1 In order to give due prominence10 to this relationship, however, we must replace the usual time co-ordinate t by an imaginary magnitude StartRoot negative 1 EndRoot dot c t proportional to it. Under these conditions, the natural laws satisfying the demands of the (special) theory of relativity assume mathematical forms, in which the time co-ordinate plays exactly the same role as the three space co-ordinates. Formally, these four co-ordinates correspond exactly to the three space co-ordinates in Euclidean geometry. It must be clear even to the non-mathematician that, as a consequence of this purely11 formal addition to our knowledge, the theory perforce gained clearness in no mean measure.
These inadequate12 remarks can give the reader only a vague notion of the important idea contributed by Minkowski. Without it the general theory of relativity, of which the fundamental ideas are developed in the following pages, would perhaps have got no farther than its long clothes. Minkowski’s work is doubtless difficult of access to anyone inexperienced in mathematics, but since it is not necessary to have a very exact grasp of this work in order to understand the fundamental ideas of either the special or the general theory of relativity, I shall leave it here at present, and revert13 to it only towards the end of Part II.
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1 shuddering | |
v.战栗( shudder的现在分词 );发抖;(机器、车辆等)突然震动;颤动 | |
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2 awakened | |
v.(使)醒( awaken的过去式和过去分词 );(使)觉醒;弄醒;(使)意识到 | |
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3 virtue | |
n.德行,美德;贞操;优点;功效,效力 | |
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4 phenomena | |
n.现象 | |
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5 briefly | |
adv.简单地,简短地 | |
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6 advent | |
n.(重要事件等的)到来,来临 | |
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7 coordinates | |
n.相配之衣物;坐标( coordinate的名词复数 );(颜色协调的)配套服装;[复数]女套服;同等重要的人(或物)v.使协调,使调和( coordinate的第三人称单数 );协调;协同;成为同等 | |
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8 transformation | |
n.变化;改造;转变 | |
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9 delta | |
n.(流的)角洲 | |
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10 prominence | |
n.突出;显著;杰出;重要 | |
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11 purely | |
adv.纯粹地,完全地 | |
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12 inadequate | |
adj.(for,to)不充足的,不适当的 | |
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13 revert | |
v.恢复,复归,回到 | |
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14 detailed | |
adj.详细的,详尽的,极注意细节的,完全的 | |
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