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Question: A friend says, "It makes no sense that Anna could turn on lights in her hands simultaneously in her frame but that they don't turn on simultaneously in another-she decides to do it, and its done." By considering the tractable, if somewhat unrealistic, situation of Anna's thought being communicated to her hands by light signals, answer this objection.

Short Answer

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Answer

It is proved that Anna could turn on lights in her hands simultaneously in her frame but that they don't turn on simultaneously in another.

Step by step solution

01

Lorentz transformation.

The Lorentz transformation defines the relationship between the two frames that move at the constant velocity and relative to each other.The frame which has a motion with a constant velocity is known as the inertial frame, and the frame that has a rotational motion with constant angular velocity in a curved path is known as the non-inertial frame.

02

Determine the formulas to prove that Anna could turn on lights in her hands simultaneously in her frame but that they don't turn on simultaneously in another.

The expression to convert the time from the frame to frame is given as follows.

t'=γv(t-vc2x) (1)

Here,t' is the time in the frame S', is the time in the frame S,is the Lorentz factor for the velocity, C is the speed of the light.

03

Prove that Anna could turn on lights in her hands simultaneously in her frame but that they don't turn on simultaneously in another.

Consider the figure which shows the position of two candles in Anna’s hand.

Calculate the time measured by the observer in the moving frame when the candle is at its position .

Substitute t1 for t and x1 for x into equation (1).

t'1=γv1-vx1c2

Calculate the time measured by the observer in the moving frame when the candle is at its position .

Substitutet'1 for t and x2 for x into equation (1).

t'2=γv1-vx2c2

Calculate the time difference between the two observations,

Δt'=t'1-t'2

Substituteγv1-vx1c2 fort'1 andγv1-vx2c2 fort'2 into the above equation.

Δt'=γv1-vx1c2-γv1-vx2c2Δt'=γv1-vx1c2-1-vx2c2Δt'=γv1-vx1c2-1+vx2c2Δt'=γvvx2-x1c2

Since the time differenceΔt'0 , therefore it is proved that Anna could turn on lights in her hands simultaneously in her frame but that they don't turn on simultaneously in another.

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Most popular questions from this chapter

Refer to Figure 2.18. (a) How long is a spaceship? (b) At what speed do the ships move relative to one another? (c) Show that Anna’s times are in accord with the Lorentz transformation equations. (d) Sketch a set of diagrams showing Anna’s complementary view of the passing of the ships. Include times in both frames.

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'=(1y)dt, where u is Anna's instantaneous speed relative to Bob. Using the result of Exercise 117(c), with g replacing Fm, 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?

What is the ratio of the relativistically correct expression for momentum to the classical expression? Under what condition does the deviation become significant?

The diagram shows Bob's view of the passing of two identical spaceship. Anna's and his own, where γv=2. The length of either spaceship in its rest frame is . What are the readings on Anna', two unlabelled clocks?

Bob is watching Anna fly by in her new high-speed plane, which Anna knows to be 60min length. As a greeting, Anna turns on two lights simultaneously, one at the front and one at the tail. According to Bob, the lights come 40nsapart.

(a) Which comes on first?

(b) How fast is the plane moving?

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