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You stand at the center of your 100m spaceship and watch Anna's identical ship pass at 0.6c. At t=0 on your wristwatch, Anna, at the center of her ship, is directly across you and her wristwatch also reads 0.

(a) A friend on your ship,24m from you in a direction towards the tail of the ship, looks at a clock directly across from him on Anna's ship. What does it read?

(b) Your friend now steps onto Anna's ship. By this very act he moves from a frame where Anna is one age to a frame where she is another. What is the difference in these ages? Explain.

(c) Answer parts (a) and (b) for a friend 24m from you but in a direction toward the front of Anna's passing ship.

(d) What happens to the reading on a clock when you accelerate toward it? Away from it?

Short Answer

Expert verified

(a) The clock directly across the friend at x=-24 m reads 60 ns.

(b) When the friend shifted to Anna's ship, her age, according to the friend, jumped forward by 60 ns.

(c) The clock directly across the friend at x=24 m reads 60 ns. When the friend shifted to Anna's ship, her age, according to the friend, jumped backward by 60 ns.

(d) Clock readings jump up when the observer accelerates toward it and jumps down when the observer accelerates away from it.

Step by step solution

01

Given data

Speed of Anna with respect to the stationary observer is,

v=0.6c
02

Lorentz transformation

Thetime interval t' measured by a moving observer at velocityv is related to the time interval t of two events measured by a stationary observer and the space interval x of the two events measured by the stationary observer as,

t'=t-vc2x1-v2c2 .....(I)

Here c is the speed of light in vacuum.

03

Step 3:Determining time in Anna's spaceship

(a)

When the clock at the mid-point of the spaceship reads t=0,the time at24 mbehind the ship also readst=0. The time at the same location at Anna's ship can be obtained from equation (I) as,

t'=00.6cc2(24 m)10.62=6×108 s=60 ns

Thus, the clock reads 60 ns.

04

Determining Anna's age jump if the friend shifts to Anna's ship

(b)

The clock at x=0 and x=24 m both read t=0. Suppose the friend shifts to Anna's ship, and the clock there reads t'=60 ns, which should also be the reading on the clock with Anna as they are synchronized.

Thus, Anna's age jumped forward by 60 ns.

05

Determining reading on the clock and Anna's age jump if the friend is toward the front of the ship

(c)

The friend is now at x=24 m. The time at the same location at Anna's ship can be obtained from equation (I) as,

t'=00.6cc2(+24 m)10.62=6×108 s=60 ns

Thus the clock reads 60 ns, which will also be the jump in Anna's age.

06

Determining the change in clock reading if the observer accelerates towards it or away from it

(d)

In the first case, the friend accelerates towards Anna when he jumps ship. Initially, Anna was moving away from him, and after the jump, Anna was at rest with respect to him. So the friend accelerated toward Anna. Here the clock reading jumped up.

In the second case, initially, Anna was moving toward the friend, and after the jump, Anna was at rest with respect to the friend. So the friend accelerated away from Anna. Here the clock reading jumped backward.

Thus, clock readings jump up when the observer accelerates toward it and jumps down when the observer accelerates away from it.

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Most popular questions from this chapter

Equation (2-30) is an approximation correct only if the gravitational time-dilation effect is small. In this exercise, it is also assumed to be small. but we still allow for a nonuniform gravitational field. We start with (2-29), based on the Doppler effect in the accelerating frame. Consider two elevations, the lower at r1 and the upper at r1+dr. Equation (2·29) becomes

f(r1+dr)f(r1)=(1-gr1drc2)

Similarly, if we consider elevationsdata-custom-editor="chemistry" r1+dr and data-custom-editor="chemistry" r1+2dr, we have

f(r1+2dr)f(r1+dr)=(1-gr1+drdrc2)

We continue the process, incrementing r by dr, until we reach r2.

f(r2)f(r2-dr)=(1-gr2-drdrc2)

Now imagine multiplying the left sides of all the equations and setting the product equal to the product of all the right sides. (a) Argue that the left side of the product is simply f(r2)/f(r1). (b) Assuming that the termgdr/c2 in each individual equation is very small. so that productsof such termscan be ignored, argue that the right side of the product is

1-1c2g(r)dr

(c) Deduceg(r) from Newton’s universal law of gravitation, then argue that equation (2-31) follows from the result, just as (2-30) does from (2-29).

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?

Derive the following expressions for the components of acceleration of an object , ax'and ay'in the frameS' in terms of its components of acceleration and velocity in the frame S.

ax'=axγv3(1-uxvc2)3ay'=ayγv2(1-uxvc2)2+axuyvc2γv2(1-uxvc2)3

An object of mass 3mo moves to the right at 0.8c.

a) Calculate its momentum and energy.

b) Using the relativistic velocity transformation, determine its velocity in a new frame of reference moving it to right at 0.5c, then using it to determine the object's momentum and energy in this new frame.

c) Verify that equations role="math" localid="1657556434416" (2-38) are satisfied.

A spaceship travels at 0.8c. As this spaceship covers 4000km from coast to coast, by how much will the time interval registered on an onboard clock differ from the time interval measured on ground?

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