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What's a decent formula for the average distance of an orbiting body, as a function of periapsis, apoapsis?

How do you calculate the average distance (over TIME) of an orbiting body from its primary, given the periapsis and apoapsis (or equivalently, the orbit's semimajor axis and its eccentricity)?

I know in abstract that the solution should be:

R_avg = ∫R(t)dt / T

where R(t) is the body's distance as a function of time; and T is its period. However, I don't think there's a closed-form solution for R(t), is there? Failing that, is there a (short) formula that gives a fair numerical approximation?

Also, my intuition is that "T" should cancel out of the final equation (i.e. R_avg should depend just on the geometry of the orbit), since the geometry uniquely determines the fraction of time that the body spends in any particular segment of the orbit.

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  • 1 decade ago
    Favorite Answer

    The answer is a(1 + e^2/2), where a is the semi-major axis and e the eccentricity.

    That is calculated in here: http://scitation.aip.org/getabs/servlet/GetabsServ... which you can find in a library.

    Online the formula is used in this article: http://iopscience.iop.org/0004-637X/592/1/555/full... see formula 8.

    So for an extreme example as Halley's comet, e= 0.93, the time averaged distance is 50% larger than the semi-major axis.

  • ?
    Lv 4
    1 decade ago

    Assuming an inverse square central field (force) acting on the bodies orbiting...

    f(r) = -k/r² k = Gm1m2

    given the differential equation of the orbit of a mass moving under a central force is:

    d²u/dθ² + u = - [/mh²u²][f(u^-1] where u = 1/r for a central force and h is the angular momentum per unit mass. h = L/m

    then the equation above becomes:

    d²u/dθ² + u = k/mh²

    A solution is:

    u = A cos(θ - θo) + k/mh²

    Constants of integration A and θo set up the initial conditions, so let θo = 0

    and we get subsituting u = 1/r that

    r = 1/(Acosθ + k/mh²)

    This is the polar equation of an orbit and can be written as:

    r = ro [1 + e]/(1 + e cosθ) where e = eccentricity and is equal to Amh²/k

    and ro = mh²/k(1 +e) when θo = 0

    Given the constant e is the eccentricity then for

    e < 1 --> the orbit is an ellipse

    e = 0 --> the orbit is a perfect circle

    e = 1 --> the "orbit" is parabolic (never comes back)

    e > 1 --> the "orbit" is hyperbolic (never comes back)

    So long as e is zero or <0 then you should be able to use the perimeter of a circle or an ellipse to calculate the distance traveled. After that all bets are off! :^)

    I remember using this stuff to calculate "TLI" for the Saturn V space program. TLI = trans lunar injection, the burn they did to increase their circular orbit to an ellipitical orbit with the moon at apogee.

    We found that if the burn provided 1% too much energy, the near stationary circular orbit about the earth would go from circular to hyperbolic, meaning they'd never come home! Of course they could correct any such factor, but it showed how delicate this stuff is.

    Source(s): BS Physics; MS EE
  • 1 decade ago

    Unfortunately, the arc-length of an ellipse is an incredibly difficult problem to solve. In fact, there is no closed-form solution.

    Here is a short formula that gives a numeric approximation if you know the two "radii" of the ellipse (semimajor and semiminor axes a and b).

    http://www.efunda.com/math/areas/EllipseGen.cfm

    For any eccentricity of 93% or less, the most error this formula could result is a 5% error.

    Most orbits of the solar system, both planets and moons, are much less eccentric than this.

  • Anonymous
    1 decade ago

    orbiting bodies dont actually orbit their primaries, thats a common mistake.... both bodies orbit the barycenter located "halfway" between the sum of their masses.

    Time is only EVER a factor of density

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