blakean87 said:
Upon discovering the Starship Titanic while doing some research about time travel, I was wondering what joules would be necessary to accelerate even faster to attempt a more severe time dilation: Namely, a 50,000kg ship to 99.999999999%C. Am I correct in my calculations that this requires app. 1x10^30 joules?
If not, what are the joules required to do so? And what would the peak wattage be if I am accelerating said ship over 1 year?
Thanks.
I assume that you're doing this as a relativistic rocketry problem. I'll call the rapidity of the rocket θ. This is related to its velocity by v=ctanh\left(\theta \right). Let's say the ship has an initial mass including fuel of m_{i} and a final mass m. It will have a ship frame exhaust port exhaust velocity of v_{ex} which relates to the specific impulse I_{sp} of the fuel by v_{ex}=gI_{sp}.
A change in the rapidity of the ship will then be given by
\Delta \theta =\frac{v_{ex}}{c}ln\left(\frac{m_{i}}{m}\right)
You find the change in the rapidity from this formula and calculate the final velocity from the rapidity according to the first equation. In the case of zero initial velocity you can compose these as
v=ctanh\left(\frac{v_{ex}}{c}ln\left(\frac{m_{i}}{m}\right) \right)
I like this version as its easy to crunch numbers on a scientific calculator, but if you want you can use log properties and the hyperbolic trig version of Euler's identities to write this without the hyperbolic trig function like at a site someone else linked.
In the case of an ideal matter anti-matter rocket v_{ex}=c.
As for the question of power, this final velocity - mass ratio relation for the rocket is independent of the flow rate at which you choose to burn it off. Burn it off how you like. However, it is common to analyse the case that you are burning off the fuel at a time dependent rate such that it accelerates at a constant "proper acceleration". This is where the occupant feel like they undergo a constant "g-force" or in otherwords, if one stood on a weight scale it would read a constant weight for the cosmonaught for the whole burn. If the proper acceleration is \alpha then the ship time rate of the mass burn relates to the proper acceleration generally by
\alpha =\frac{v_{ex}}{m}\frac{dm}{dt'}, and for constant proper acceleration this integrates to result in
\alpha \frac{\Delta t'}{c} =\frac{v_{ex}}{c}ln\left(\frac{m_{i}}{m}\right)
You can then replace this into the equation for the velocity to get the velocity as a function of ship time for constant proper acceleration. If you want more information about this, just let me know.