Difference between revisions of "Alcubierre Warp Drive"
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+ | ==Stuff from Sonny White's Paper== | ||
<math>\LARGE | <math>\LARGE | ||
ds^2 = -c^2dt^2+\left(dx - v_s\left(t\right)f\left(r_s\right)dt\right)^2+dy^2+dz^2 | ds^2 = -c^2dt^2+\left(dx - v_s\left(t\right)f\left(r_s\right)dt\right)^2+dy^2+dz^2 | ||
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− | ==Other Stuff== | + | ===Other Stuff=== |
<math>\LARGE | <math>\LARGE | ||
ds^2 = \left(v_s^2f\left(r_s\right)^2-1\right)\left(dt-\frac{v_sf\left(r_s\right)}{v_s^2f\left(r_s\right)^2-1}\right)^2-dx^2+dy^2+dz^2 | ds^2 = \left(v_s^2f\left(r_s\right)^2-1\right)\left(dt-\frac{v_sf\left(r_s\right)}{v_s^2f\left(r_s\right)^2-1}\right)^2-dx^2+dy^2+dz^2 | ||
</math> | </math> | ||
+ | |||
+ | ==The Real Deal== | ||
+ | Energy density at radial position ''r<sub>s</sub>'': | ||
+ | |||
+ | <math>\LARGE | ||
+ | T^{00} = \frac{-v_s^2\rho^2}{32\pi r_s^2}\left(\frac{df}{dr_s}\right)^2 | ||
+ | </math> | ||
+ | |||
+ | Where ''ρ'' is the vacuum energy density (~6E-10 J/m<sup>3</sup>) and ''v<sub>s</sub>'' is the velocity of the warp bubble. ''df/dr<sub>s</sub>'' is the derivative of ''f(r<sub>s</sub>)'', above. | ||
+ | |||
+ | Total energy density is calculated by integrating ''T<sup>00</sup>'' for values of ''r<sub>s</sub>'' from 0 to ''R+σ'' |
Revision as of 15:03, 4 December 2012
Stuff from Sonny White's Paper
<math>\LARGE ds^2 = -c^2dt^2+\left(dx - v_s\left(t\right)f\left(r_s\right)dt\right)^2+dy^2+dz^2 </math>
This uses the familiar coordinates <math>\left(t, x, y, z\right)</math> and curve <math>x = x_s\left(t\right), y = 0, z=0</math> where x is analogous to what is commonly referred to as a spacecraft's trajectory. <math>r_s</math> is the "radial position in the commoving spherical space around the spacecraft's origin."
Sigma and R are arbitrary values that control the bubble thickness and size of the bubble, respectively.
<math>\LARGE
f\left(r_s\right) = \frac{tanh\left(\sigma\left(r_s+R\right)\right)-tanh\left(\sigma\left(r_s-R\right)\right)}{2tanh\left(\sigma R\right)}
</math>
Courtesy Mouse:
<math>\LARGE
\frac{df}{dr_s} = \frac{2tanh\left(\sigma R\right)\left(\sigma sech^2\left(\sigma r_s+\sigma R\right) - \sigma sech^2\left(\sigma r_s - \sigma R\right)\right)}{4tanh^2\left(\sigma R\right)}
</math>
Actual energy density:
<math>\LARGE
T^{00} = -1\frac{1}{8\pi}\frac{v_s^2\rho^2}{4r_s^2}\left(\frac{df}{dr_s}\right)^2
</math>
- <math>\rho</math> is the mass-energy density (kg/m^3)
Other Stuff
<math>\LARGE ds^2 = \left(v_s^2f\left(r_s\right)^2-1\right)\left(dt-\frac{v_sf\left(r_s\right)}{v_s^2f\left(r_s\right)^2-1}\right)^2-dx^2+dy^2+dz^2 </math>
The Real Deal
Energy density at radial position rs:
<math>\LARGE T^{00} = \frac{-v_s^2\rho^2}{32\pi r_s^2}\left(\frac{df}{dr_s}\right)^2 </math>
Where ρ is the vacuum energy density (~6E-10 J/m3) and vs is the velocity of the warp bubble. df/drs is the derivative of f(rs), above.
Total energy density is calculated by integrating T00 for values of rs from 0 to R+σ