# Dissertation Le Corps Transform

Now imagine viewing this from a faster train overtaking the clock train—from this view, the front clock will be the first to start.The important point is that although these events appear to occur in a different order in a different frame, neither of them could be the cause of the other, so cause and effect are not switched around. Let us try to visualize the surface in four-dimensional space described by the outgoing shell of light from a single flash, This means the surface is a cone with its point at the origin.

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Also a worksheet for pupils to match words to pictures, and two sets of cards - either to play as pelmanism or snap / go fish, matching picture to picture or picture to word.

In other words, we shall derive the Lorentz transformations—which are just the equations giving the four coordinates of an event in one inertial frame in terms of the coordinates of the same event in another inertial frame.

We take ) O′ flashes a bright light, which she observes to create an expanding spherical shell of light, centered on herself (imagine it’ s a slightly foggy day, so she can see how the ripple of light travels outwards).

It should be mentioned that this lack of synchronization as viewed from another frame only occurs for clocks separated in the direction of relative motion.

Consider two clocks some distance apart on the axis of S′.

“I know I’m not good at writing so I keep putting it off”.

“I know I’m good at writing so I can leave it to later”.

If they are synchronized in S′ by both being started by a flash of light from a bulb half way between them, it is clear that as viewed from S the light has to go the same distance to each of the clocks, so they will still be synchronized (although they will start later by the time dilation factor).

Let us now suppose that O′ and her crew observe a small bomb to explode in S′ at -axis).