Is the Travel Time to Reach the Speed of Light Really Only 2 Years?

schaefera
Messages
208
Reaction score
0
http://scienceblogs.com/startswithabang/2011/06/01/striving-for-the-speed-of-ligh/

In this article, the author claims that it would take a little over 1.25 years to reach 90% the speed of light if we accelerate at 1g.

However, if I let F=dp/dt, where p=γmv, and then integrate F with respect to t (assuming F=mg), I get that the velocity, v, will be reached at the time:

t=v/sqrt(g^2-g^2*t^2/c^2)... and plugging v=.9c into this, I get the result that it should take about 2 years and a day to reach the speed of .9c.

Whose calculation is wrong? If it is mine, where did I go wrong, and how can I correct it in my expression for time as a function of velocity?
 
Physics news on Phys.org
According to http://math.ucr.edu/home/baez/physics/Relativity/SR/rocket.html article, it looks like you're both right. He is calculating the Proper Time, T, experienced by the traveler and you are calculating the Earth time in the non-accelerating frame.
 
Thanks for the link-- it's great!

When I try to convert between measured time, t, and proper time, T, though I seem to run into a problem. I know that T=∫dT=∫(1/γ)dt. And since v=(gt)/sqrt(1+(gt/c)^2), I can plug this in and get a slightly nasty integral. After a lot of substitution, I end up wanting to integrate sec(u) du between 0 and arctan(gf/c) where f is the final time. I get something nasty with a natural log, but it comes out numerically to give me about 1.4 years which I'll say is where they rounded to get a year and a quarter. Thanks!
 
Last edited:
Using the proper time that the author of that article calculates, would that time be the actual time experience by a traveler, or merely the time an earth-bound observer would measure when using the proper equations to convert his time into the moving ship's frame?

For example, I calculate that the Earth would measure 5.93 years for a trip to the nearest star while a traveler would measure 3.56 years. But does this exhibit the usual reciprocity of special relativistic calculations (eg traveler measures 5.93 and calculates 3.56 for the earth), or does the acceleration in his case negate the symmetry? Does a traveler really only age 3.56 years despite feeling like time runs normally for him?
 
schaefera said:
Does a traveler really only age 3.56 years despite feeling like time runs normally for him?

yes, because the amount of time that runs normally for him is 3.56 years. He sees 3.56 years tick by, by looking at his wristwatch, counting his heartbeats, watching paint dry... As long he's only looking at the local phenomena aboard his spaceship, where only 3.56 years passes. That's proper time, the time that he experiences on his path through spacetime.

Someone else taking a different path through spacetime will measure a different proper time on their path, even if the starting and ending points are the same. They're measuring proper time along the path that they took; it's a different path so in general it has a different proper time.

An analogy (and I must stress that this is an analogy - don't take it too seriously!): Suppose you and I are are both driving in our own cars between points A and B. Before we leave, we compare the odometer readings. We compare again at some time after we've arrived at the destination, and we see that my car has covered 600 miles and your car has covered only 500 miles. We expect that my car has experienced a bit more wear and is a bit closer to its next oil change, but we don't think anything strange has happened - we just conclude that you took a shorter route. We also still have no idea how far apart the two cities "really" are, although we do know that they are not more than 500 miles apart.

We just aren't used to thinking about time in the same way... we have this mental model that there's some giant clock up in the sky that we're all sharing. There isn't.
 
Last edited:
Thread 'Can this experiment break Lorentz symmetry?'
1. The Big Idea: According to Einstein’s relativity, all motion is relative. You can’t tell if you’re moving at a constant velocity without looking outside. But what if there is a universal “rest frame” (like the old idea of the “ether”)? This experiment tries to find out by looking for tiny, directional differences in how objects move inside a sealed box. 2. How It Works: The Two-Stage Process Imagine a perfectly isolated spacecraft (our lab) moving through space at some unknown speed V...
Does the speed of light change in a gravitational field depending on whether the direction of travel is parallel to the field, or perpendicular to the field? And is it the same in both directions at each orientation? This question could be answered experimentally to some degree of accuracy. Experiment design: Place two identical clocks A and B on the circumference of a wheel at opposite ends of the diameter of length L. The wheel is positioned upright, i.e., perpendicular to the ground...
In Philippe G. Ciarlet's book 'An introduction to differential geometry', He gives the integrability conditions of the differential equations like this: $$ \partial_{i} F_{lj}=L^p_{ij} F_{lp},\,\,\,F_{ij}(x_0)=F^0_{ij}. $$ The integrability conditions for the existence of a global solution ##F_{lj}## is: $$ R^i_{jkl}\equiv\partial_k L^i_{jl}-\partial_l L^i_{jk}+L^h_{jl} L^i_{hk}-L^h_{jk} L^i_{hl}=0 $$ Then from the equation: $$\nabla_b e_a= \Gamma^c_{ab} e_c$$ Using cartesian basis ## e_I...
Back
Top