The Twin Paradox

The Twin Paradox

An intriguing consequence of time dilation is that a space traveler moving at a high velocity relative to the Earth would age less than her Earth-bound twin. Imagine the astronaut moving at such a velocity that \(\gamma =\text{30}\text{.}0\), as in this figure. A trip that takes 2.00 years in her frame would take 60.0 years in her Earth-bound twin’s frame. Suppose the astronaut traveled 1.00 year to another star system. She briefly explored the area, and then traveled 1.00 year back. If the astronaut was 40 years old when she left, she would be 42 upon her return. Everything on the Earth, however, would have aged 60.0 years. Her twin, if still alive, would be 100 years old.

The situation would seem different to the astronaut. Because motion is relative, the spaceship would seem to be stationary and the Earth would appear to move. (This is the sensation you have when flying in a jet.) If the astronaut looks out the window of the spaceship, she will see time slow down on the Earth by a factor of \(\gamma =\text{30}\text{.}0\). To her, the Earth-bound sister will have aged only 2/30 (1/15) of a year, while she aged 2.00 years. The two sisters cannot both be correct.

As with all paradoxes, the premise is faulty and leads to contradictory conclusions. In fact, the astronaut’s motion is significantly different from that of the Earth-bound twin. The astronaut accelerates to a high velocity and then decelerates to view the star system. To return to the Earth, she again accelerates and decelerates. The Earth-bound twin does not experience these accelerations. So the situation is not symmetric, and it is not correct to claim that the astronaut will observe the same effects as her Earth-bound twin.

If you use special relativity to examine the twin paradox, you must keep in mind that the theory is expressly based on inertial frames, which by definition are not accelerated or rotating. Einstein developed general relativity to deal with accelerated frames and with gravity, a prime source of acceleration. You can also use general relativity to address the twin paradox and, according to general relativity, the astronaut will age less. Some important conceptual aspects of general relativity are discussed in General Relativity and Quantum Gravity of this course.

In 1971, American physicists Joseph Hafele and Richard Keating verified time dilation at low relative velocities by flying extremely accurate atomic clocks around the Earth on commercial aircraft. They measured elapsed time to an accuracy of a few nanoseconds and compared it with the time measured by clocks left behind. Hafele and Keating’s results were within experimental uncertainties of the predictions of relativity. Both special and general relativity had to be taken into account, since gravity and accelerations were involved as well as relative motion.

Check Your Understanding

1. What is \(\gamma \) if \(v=0\text{.650}c\)?

Solution

\(\gamma =\cfrac{1}{\sqrt{1-\cfrac{{v}^{2}}{{c}^{2}}}}=\cfrac{1}{\sqrt{1-\cfrac{(0\text{.}\text{650}c{)}^{2}}{{c}^{2}}}}=1\text{.}\text{32}\)

2. A particle travels at \(1\text{.}\text{90}×{\text{10}}^{8}\phantom{\rule{0.25em}{0ex}}\text{m/s}\) and lives \(2\text{.}\text{10}×{\text{10}}^{-8}\phantom{\rule{0.25em}{0ex}}s\) when at rest relative to an observer. How long does the particle live as viewed in the laboratory?

Solution

\(\Delta t=\cfrac{{\Delta }_{t}}{\sqrt{1-\cfrac{{v}^{2}}{{c}^{2}}}}=\cfrac{2\text{.}\text{10}×{\text{10}}^{-8}\phantom{\rule{0.25em}{0ex}}\text{s}}{\sqrt{1-\cfrac{(1\text{.}\text{90}×{\text{10}}^{8}\phantom{\rule{0.25em}{0ex}}\text{m/s}{)}^{2}}{(3\text{.}\text{00}×{\text{10}}^{8}\phantom{\rule{0.25em}{0ex}}\text{m/s}{)}^{2}}}}=2\text{.}\text{71}×{\text{10}}^{-8}\phantom{\rule{0.25em}{0ex}}\text{s}\)

This lesson is part of:

Special Relativity

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