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Relativistic Velocity Transformation

相对论速度变换

No two objects can have a relative velocity greater than c! But what if I observe a spacecraft traveling at 0.8c and it fires a projectile which it observes to be moving at 0.7c with respect to it!? Velocities must transform according to the Lorentz transformation, and that leads to a very non-intuitive result called Einstein velocity addition.

没有两个物体可以有超过光速的相对速度!但如果我观察一个以0.8c速度飞行的航天器,并且它发射出一个以0.7c速度运动的弹体(相对于它自己),那么速度必须按照洛伦兹变换进行变换,这会导致一个非常非直观的结果,称为爱因斯坦速度相加。

Just taking the differentials of these quantities leads to the velocity transformation. Taking the differentials of the Lorentz transformation expressions for x' and t' above gives

仅仅对这些量求微分就得到速度变换。对上述洛伦兹变换表达式中的x'和t'求微分就得到

Putting this in the notation introduced in the illustration above:

The reverse transformation is obtained by just solving for u in the above expression. Doing that gives

逆变换 simply 通过解上述表达式中的 u 得到。这样做得到

Applying this transformation to the spacecraft traveling at 0.8c which fires a projectile which it observes to be moving at 0.7c with respect to it, we obtain a velocity of 1.5c/1.56 = 0.96c rather than the 1.5c which seems to be the common sense answer.

将这一变换应用于以0.8c速度飞行的航天器,该航天器观察到一个弹体以0.7c相对于它运动,我们得到弹体的速度为1.5c/1.56 = 0.96c,而不是直觉上似乎合理的1.5c。
Basic application
基本应用
Relativistic relative velocity
相对论性相对速度
Velocity of projectile, external observer
projectile 的速度,外部观察者
Velocity of projectile from target
从目标发射的弹体速度
将此内容放入上述示意图中引入的符号体系中:
Index
索引
 
HyperPhysics***** Relativity
HyperPhysics ***** 相对论
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