True anomaly

From Wikipedia, the free encyclopedia

In astronomy, the true anomaly (T\,\!, also written v\) is the angle between the direction z-s of periapsis and the current position p of an object on its orbit, measured at the focus s of the ellipse (the point around which the object orbits). In the diagram below, true anomaly is the angle z-s-p.

Image:Kepler's-equation-scheme.png

For elliptic orbits true anomaly T\,\! can be calculated from orbital state vectors as:

T = \arccos { {\mathbf{e} \cdot \mathbf{r}} \over { \mathbf{\left |e \right |} \mathbf{\left |r \right |} }} (if \mathbf{r} \cdot \mathbf{v} < 0 then replace T by 2π − T)

where:


For circular orbits this can be simplified to:

T = \arccos { {\mathbf{n} \cdot \mathbf{r}} \over { \mathbf{\left |n \right |} \mathbf{\left |r \right |} }} (if \mathbf{n} \cdot \mathbf{v} >0 then replace T by 2π − T)

where:

  • \mathbf{n} is vector pointing towards the ascending node (i.e. the z-component of \mathbf{n} is zero).

For circular orbits with the inclination of zero this can be simplified further to:

T = \arccos { r_x  \over { \mathbf{\left |r \right |}}} (if v_x\ > 0 then replace T by 2π − T)

where:

The relation between T and E, the eccentric anomaly, is:

\cos{T} = {{\cos{E} - e} \over {1 - e \cdot \cos{E}}},\,

or equivalently

\tan{T \over 2} = \sqrt{{{1+e} \over {1-e}}} \tan{E \over 2}.

The relations between the radius (position vector magnitude) and the anomalies are:

r = a \left ( 1 - e \cdot \cos{E} \right )\,\!

and

r = a{(1 - e^2) \over (1 + e \cdot \cos{T})}\,\!

where a is the orbit's semi-major axis (segment cz). Note that z is the periapsis (closest approach to the focus or object being orbited) and also one of two points where the semi-major axis (furthest distance from the centre of the ellipse) can be measured, the other point being the apoapsis (furthest distance from the focus being orbited and 180 degrees around from the periapsis).

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