For the situation given in Exercise 22, find the Lorentz transformation matrix from Bob’s frame to Anna’s frame, then solve the problem via matrix multiplication.

Short Answer

Expert verified

The Lorentz transformation matrix is 5300-4301000010-430053.

Via matrix multiplication, the value of x' is gathered as173Iy=5.67Iy and the value of t' is gathered as -103yr=-3.33yr.

Step by step solution

01

Given data

Anna is in a spaceship moving away from Earth at v=0.8c

02

Significance of the Lorentz transformation

The Lorentz transformation mainly describes the time and the space coordinate of one reference frame. It also describes the relationship amongst two frames of coordinates.

03

Determination of the Lorentz transformation

The equation of the Lorentz transformation is expressed as:

x'y'z'ct'=yv00-yvvc01000010-yvvc00yvx'y'z'ct'

…(i)

Here, the value of y08cis expressed as:

y0.8c=11-0.8c2c2=11-0.64c2c2=11-0.64=53

Here, the value of -y0.8cvcis expressed as:

-y0.8cvc=-53×0.8=-43Substitutethevaluesintheequation(i),thematrixisexpressedas:x'y'z'ct'=5300-4301000010-4300535300-4301000010-4300535Iy00c2yr=25Iy3+-8Iy300-20cIy3+10cyr3=17Iy300-10cyr3x'y'z'ct'=17Iy300-10cyr3

From the above matrix, the value of x' is gathered as173Iy=5.67Iyand the value of t' is gathered as -103yr=-3.33yr..

Thus, the Lorentz transformation matrix is 5300-4301000010-430053.

Via matrix multiplication, the value of x' is gathered as 173Iy=5.67Iyand the value of t' is gathered as -103yr=-3.33yr.

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Question: Equation (2-38) show that four-momentum of a particle obeys a Lorentz transformation. If we sum momentum and energy over all particles in a system, we see that the total momentum and energy also constitute a four-vector. It follows that (Etotal/c)2-Ptotal2 is the same quantity in any frame of reference. Depending on what is known, this can be a quicker route to solving problems than writing out momentum and energy conservation equations. In the laboratory frame, a particle of mass m and energy Ei collide with another particle of mass initially stationary, forming a single object of mass . (a) Determine the frame of reference where the after-collision situation is as simple as possible, then determine the invariant in that frame. (b) Calculate the invariant before the collision in the laboratory frame in terms of M and Ei . (You will need to use Ei2/c2-p2=m2c2 for the initially moving particle to eliminate its momentum.) Obtain an expression for M in terms of m and Ei . (c) Write out momentum and energy conservation in the laboratory frame, using uf for the speed of the initially moving particle and for the speed of the final combined particle. Show that they give the same result for M in terms of m and Ei. (Note: The identity γu2u2=γu2c2-c2 will be very handy.)

In Example 2.5, we noted that Anna could go wherever she wished in as little time as desired by going fast enough to length-contract the distance to an arbitrarily small value. This overlooks a physiological limitation. Accelerations greater than about 30gare fatal, and there are serious concerns about the effects of prolonged accelerations greater than 1g. Here we see how far a person could go under a constant acceleration of 1g, producing a comfortable artificial gravity.

(a) Though traveller Anna accelerates, Bob, being on near-inertial Earth, is a reliable observer and will see less time go by on Anna's clock (dt')than on his own (dt).Thus, dt'=(1/γ)dt, where u is Anna's instantaneous speed relative to Bob. Using the result of Exercise 117(c),with g replacing F/m, substitute for u,then integrate to show that

t=cgsinhgt'c

(b) How much time goes by for observers on Earth as they “see” Anna age 20 years?

(c) Using the result of Exercise 119, show that when Anna has aged a time t’, she is a distance from Earth (according to Earth observers) of

x=c2g(coshgt'c-1)

(d) If Anna accelerates away from Earth while aging 20 years and then slows to a stop while aging another 20. How far away from Earth will she end up and how much time will have passed on Earth?

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