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It will get trickier for interstellar distances. In Newtonian mechanics v = at, so it'd take rather less than the usual yr to reach c at one g acceleration. But relativity would not allow for that, we can only get near c.
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In the stationary observer's viewpoint the traveler's amount of acceleration would sluggish since they approached the velocity of light. The traveler would see no transform involving their pace along with the speed of light. As an alternative they would encounter time at an progressively slower fee which might effectively induce the distance to your destination to become shorter.
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James JenkinsJames Jenkins 27.2k2323 gold badges108108 silver badges242242 bronze badges $endgroup$ three four $begingroup$ "1g of thrust" pointed straight up will balance gravity, and end in you floating. "1g" (as I go through it), could be the acceleration caused by the Earth's gravity; if which here is how you actually determine it, then your acceleration decreases as you can get further more (and 'experience a lot less pull') from Earth.
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What on earth is the biggest human body from the solar system we could meaningfully and correctly modify the orbit of? two
$begingroup$ When you've got the Strength for a relentless 1G thrust, just how long would it not choose to obtain on the planets within our solar method? How long for your 5 closest solar methods?
But that point is from the viewpoint of stationary observers for the departure issue. The excursion's period with the traveler's viewpoint will be less mainly because of the time dilation influence predicted by Einstein's Idea of Relativity. The better the space, the better the pace within the stationary observer's viewpoint.
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one $begingroup$ @Mark not quite legitimate. In fact, for those who notice matters slipping in regular gravity, you still are not able to see them go beyond pace of light, indicating that Newtonian physics isn't going to maintain at the same time as observed by the ship. $endgroup$
HopDavidHopDavid 16k4444 silver badges8080 bronze badges $endgroup$ nine twenty $begingroup$ Your "add somewhat more than the usual calendar year for every lightyear length" is proper for an outdoor observer, but for somebody aboard the ship, the Newtonian product is right for all distances (as measured before beginning acceleration): Lorentz contraction will shrink the universe all through journey to give the looks of Newtonian physics. $endgroup$
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