How Does Time Dilation Affect Clock Readings in Different Frames?

Click For Summary
SUMMARY

The discussion centers on the effects of time dilation on clock readings between two planets, A and B, and a spaceship traveling at speed v. When the spaceship synchronizes its clock with the clocks on planets A and B, it experiences time differently due to relativistic effects. Specifically, when the spaceship reaches planet B, the clock on B reads L/v, while the spaceship's clock reads L/γv, where γ is the Lorentz factor. The resolution of the apparent paradox lies in the non-simultaneity of clock resets between the spaceship and the planets, leading to different time perceptions.

PREREQUISITES
  • Understanding of special relativity principles
  • Familiarity with Lorentz transformation equations
  • Knowledge of time dilation effects in relativistic physics
  • Basic grasp of synchronization of clocks in different reference frames
NEXT STEPS
  • Study the Lorentz transformation in detail
  • Explore the concept of simultaneity in special relativity
  • Learn about the implications of time dilation on moving observers
  • Investigate practical applications of time dilation in modern physics
USEFUL FOR

Students of physics, educators teaching special relativity, and anyone interested in the implications of time dilation in relativistic scenarios.

bigevil
Messages
77
Reaction score
0

Homework Statement



Two planets A and B are at rest with respect to each other and are L apart in this frame. They have synchronised clocks. A spaceship flies at speed v with respect to planet A and synchronises its clock with A-B.

We know that when the spaceship reaches B, B's clock reads L/v and the ship's clock reads L/γv. How would someone account for the fact that B's clock reads L/v, which is more than its own L/γv, considering that the spaceship sees B's clock as running slow.

Homework Equations



I'm not sure if I got the correct solution, please help me to check if the reasoning is correct.

Let the frame A-B measure (x,y,z,t).
Let the ship measure coordinates (x',y',z',t').

Using the Lorentz transformation for time,

[tex]t' = \gamma (t - vL/c^2)[/tex]

When A-B resets its clock at zero (t=0), t' registers [tex]- vL\gamma / c^2[/tex]. Relative to the time of A-B, the ship's clock runs at vLγ/(c*c) slower.

When the ship passes B, time at AB is t = L/v. Then,

[tex]\gamma (\frac{L}{v} - \frac{Lv}{c^2}) = \frac{L}{\gamma v}[/tex].

-------------
My solution:

When I reset my clock at A, this event is not simultaneous with the time reset at the two planets. In fact, the planets have a "head start" of vLγ/c^2. In the planet's time it takes L/v for me to reach there. In my time, to adjust for the head start, the time to reach B is L/γv.

The resolution of the paradox (that my clock is slower on my ship than the planet's, although due to time dilation, I should read the planet's clock as slower) lies in the assumption that the time reset of the A-B system and the reset of the ship are simultaneous, but they are not.
 
Physics news on Phys.org
bigevil said:
The resolution of the paradox (that my clock is slower on my ship than the planet's, although due to time dilation, I should read the planet's clock as slower) lies in the assumption that the time reset of the A-B system and the reset of the ship are simultaneous, but they are not.

Hi bigevil! :smile:

this is all very confusing :redface:

what's all this about "resetting"? :confused:

i can't see whether you've got it or not …

the important question is whether times on A and B which are simultaneous for A (or B) are also simultaneous for the spaceship :wink:
 

Similar threads

  • · Replies 12 ·
Replies
12
Views
3K
  • · Replies 67 ·
3
Replies
67
Views
5K
  • · Replies 1 ·
Replies
1
Views
1K
Replies
10
Views
3K
  • · Replies 6 ·
Replies
6
Views
5K
  • · Replies 2 ·
Replies
2
Views
2K
Replies
11
Views
3K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
Replies
6
Views
3K