2 3/2 u uvx 0; -0,(1-4 (1--2--²- a'x=a₁|1 2 -3

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Chapter30: Atomic Physics
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Problem 3CQ: If atoms exist, why can't we see them with visible light?
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Consider two inertial reference frames S and S' in standard orientation so that S' moves along the positive x-axis with constant velocity u relative to S. A particle moves relative to frame S along the x-axis with instantaneous velocity Vx and instantaneous acceleration ax.

(a) Show that the instantaneous acceleration a's of the particle in frame S' is 2 3/2 и, a' =a 1- 1

 

(b) The proper acceleration a of a particle at a given point P on its world line is defined to be the acceleration of the particle relative to a co-moving inertial frame at P. By definition, the instantaneous velocity of the particle is zero relative to the co-moving frame. As the velocity of the particle changes along the world line, we can imagine there exist different co-moving inertial frames at different points along the world line of the particle. Now suppose u is the instantaneous velocity of the particle measured by a fixed laboratory inertial frame S. Derive the instantaneous acceleration ax of the particle frame S in terms of a and u.

(c) In special relativity, the acceleration of a particle is said to be uniform if the proper acceleration of the particle remains a constant value along its world line. Show that, with an appropriate choice of initial conditions, the world line of the particle in frame S is given by x?-(ct)? c)2=l&). - where (t, x) are the coordinates in frame S.

x²-(c)²=(2²) ².
a
Transcribed Image Text:x²-(c)²=(2²) ². a
2 3/2
-3
uvx
0²,=0,(1-4 | *(1-UV.) ³.
a' a 2
Transcribed Image Text:2 3/2 -3 uvx 0²,=0,(1-4 | *(1-UV.) ³. a' a 2
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