Relativistic motion of a magnetic sail

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SUMMARY

The discussion centers on the development of the magnetic sail for interplanetary flight by Robert Zubrin and Dana Andrews. Key equations of motion are presented, including the classical equation V = Vo/(1 + Vo^(1/3)*k*t)^3, which describes velocity as a function of time and acceleration as a = -3*V^(4/3)*k. The participants explore the transition from classical to relativistic equations of motion, suggesting that rapidity may replace velocity and proper time may replace time. Additionally, the self-acceleration of the magnetic sail is defined by the equation D/M= 0.59 (μ0ρ2V4Rm/I)1/3(J/ρm), emphasizing the importance of magnetic field strength in deflecting ion flow.

PREREQUISITES
  • Understanding of classical mechanics and equations of motion
  • Familiarity with relativistic physics concepts, particularly rapidity
  • Knowledge of magnetic fields and their interaction with charged particles
  • Basic understanding of ion flow dynamics and magnetic braking techniques
NEXT STEPS
  • Study the principles of relativistic motion and how they apply to magnetic sails
  • Explore the mathematical derivation of relativistic equations from classical equations
  • Research the effects of magnetic field strength on ion flow deflection
  • Review Giovanni Vulpetti's 1990 paper on magnetic braking for additional insights
USEFUL FOR

Aerospace engineers, physicists, and researchers interested in advanced propulsion systems and relativistic motion applications in space travel.

qraal
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Hi All

Robert Zubrin and Dana Andrews developed the magnetic-sail for use in interplanetary flight and deccelerating from interstellar speeds.

The basic classical equation of motion is this...

V = Vo/(1 + Vo^(1/3)*k*t)^3

...where k is a constant, t is time since decceleration began, Vo is initial velocity, and V final velocity.

It's pretty straight forward to then integrate to find displacement...

s = (1/2k)*(Vo^(2/3)-V^(2/3))

...remembering that V is V(t), a function of t.

Differentiating V(t) gives...

a = -3*Vo^(4/3)*k/(1 + Vo^(1/3)*k*t)^4

...but (V/Vo)^(1/3) = 1/(1+Vo^(1/3)*k*t) so the equation simplifies to...

a = -3*V^(4/3)*k

Those are the basic equations of motion, classically. How would I go about turning them into relativistic equations of motion? Would V(t) need to be rapidity, and t become <tau>?
 
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Hi qraal! Welcome to PF! :smile:

(have a gamma: γ and try using the X2 and X2 tags just above the Reply box :wink:)
qraal said:
V = Vo/(1 + Vo^(1/3)*k*t)^3

Those are the basic equations of motion, classically. How would I go about turning them into relativistic equations of motion? Would V(t) need to be rapidity, and t become <tau>?

That equation looks as if it comes from a more basic differential equation …

what is that? …

that's the one you'll have to convert, by changing momentum to mvγ and energy to mγ :smile:
 
Hi tiny-tim

Thanks for the tips on formatting. Very handy.

So the basic equation is dV/dt = -3kV4/3 and most of the tricky stuff is in that k factor. Zubrin's initial equation is...

D/M= 0.59 (μ0ρ2V4Rm/I)1/3(J/ρm)

...which is the self-acceleration of the magnetic-sail in an ion flow of density ρ and relative velocity V. Thus if the sail is doing the moving then the acceleration is negative to the direction of motion. I is current, μ0 = 4π x 10-7, and (J/ρm) the maximum current density of the loop.

I think my main question is just how powerful the magnetic field needs to be at high speeds to actually deflect the ion flow as required and not just have it fly past the loop, compressing the generated magnetosphere. I have a 1990 paper by Giovanni Vulpetti on magnetic braking which I should probably study a bit more.
 

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