Monday, April 5, 2010

Course 3 on Lorentz-Four-Contractions, Last Test, Part 1

1) if an object is traveling along a specific axis in general at .5c, describe what strings will be contracted according to the equation I gave, which strings would not be contracted at all lengthwise as a unit, and which strings would contract moderately in the globally distinguishable.

2) Why does matter and kinetic energy contract relative to light?

3) What are the basic equations for Lorentz-Four-Contractions?

4) If an object were to travel at .8c, how would its length, width, mass, and time be effected by a stander by?

5) Why can't a mass travel at light speed if it has a Kaluza-Klein light-cone-gauge topology?

6) A perfect "X" of two strings travels in the direction of the gap between them at .8c, describe the contraction of both lines that comprise the "X." (The strings would never collide.)

7) If an object is traveling in a different direction than that direction that is changing at close to light speed, yet certain of its strings are moving at the quicker string's speed, how will that object contract quantitatively?

8) Will any spherical object Lorentz-Contract uniformally if it is traveling in one direction at less than light speed? Why?

No comments: