Relativistic motion of a magnetic sail

qraal
Messages
787
Reaction score
3
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>?
 
Physics news on Phys.org
Welcome to PF!

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.
 
I started reading a National Geographic article related to the Big Bang. It starts these statements: Gazing up at the stars at night, it’s easy to imagine that space goes on forever. But cosmologists know that the universe actually has limits. First, their best models indicate that space and time had a beginning, a subatomic point called a singularity. This point of intense heat and density rapidly ballooned outward. My first reaction was that this is a layman's approximation to...
Thread 'Dirac's integral for the energy-momentum of the gravitational field'
See Dirac's brief treatment of the energy-momentum pseudo-tensor in the attached picture. Dirac is presumably integrating eq. (31.2) over the 4D "hypercylinder" defined by ##T_1 \le x^0 \le T_2## and ##\mathbf{|x|} \le R##, where ##R## is sufficiently large to include all the matter-energy fields in the system. Then \begin{align} 0 &= \int_V \left[ ({t_\mu}^\nu + T_\mu^\nu)\sqrt{-g}\, \right]_{,\nu} d^4 x = \int_{\partial V} ({t_\mu}^\nu + T_\mu^\nu)\sqrt{-g} \, dS_\nu \nonumber\\ &= \left(...
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...

Similar threads

Back
Top