Angle of the Sun above orbit plane on satellite-centered celestial sphere

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Discussion Overview

The discussion revolves around calculating the maximum angle of the Sun above the orbital plane of a satellite, particularly in relation to eclipse-free orbits. Participants explore the implications of satellite altitude and inclination on this angle, as well as the effects of Earth's oblateness on satellite orbits, specifically sun-synchronous orbits.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant seeks to calculate the Sun's maximum angle above the orbital plane using a satellite-centered celestial coordinate system, noting potential issues with high inclination angles exceeding 90 degrees.
  • Another participant clarifies that orbits with inclination greater than 90 degrees are retrograde, referencing sun-synchronous satellites with inclinations around 98 degrees.
  • A third participant introduces the concept of nodal precession due to Earth's oblateness, providing a mathematical expression for the precession rate and its dependence on various parameters.
  • A later reply discusses the implications of nodal precession on the eclipse duration for sun-synchronous satellites, indicating that the effect varies based on the satellite's path relative to the Earth's orbit around the Sun.
  • Participants inquire about visualization tools to better understand satellite orbit behaviors, with one suggesting STK as a potential resource.

Areas of Agreement / Disagreement

Participants express differing views on the implications of satellite inclination and the effects of Earth's oblateness, indicating that multiple competing perspectives remain. The discussion does not reach a consensus on the maximum angle calculation or the constancy of eclipse durations for sun-synchronous orbits.

Contextual Notes

Limitations include assumptions about the circularity of Earth's orbit and the specific conditions under which eclipse durations are considered constant. The discussion also highlights the complexity of orbital mechanics and the need for precise definitions and parameters.

gnurf
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I'm trying to show that for certain combinations of altitude and inclination there will be periods of the year where a satellite has eclipse-free orbits. Using a satellite-centered celestial coordinate system, in which the orbit plane is the equator and the direction of Earth is fixed along the x-axis, how do I calculate the Sun's maximum angle above the orbit plane?

I know the altitude, and thus the angular radius of the Earth disc on the sphere. In my book, to get the maximum angle of the Sun above the orbital plane, they simply take the sum of the orbit inclination and the angle between the ecliptic and the Earth's equator (23 deg). This is fine until the orbit inclination > 67 degs, for which the max sun angle would exceed 90 degrees -- which doesn't make sense (to me) if I understand the geometry in the figures of my book correctly. E.g., what if the orbit is a LEO orbit with 100 degrees inclination?
 
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An orbit with inclination > 90 degrees is a retrograde orbit. For example, a lot of LEO Earth observation satellites are in sun synchronous orbits with inclination of about 98 degrees.
 
Speaking of sun synchronous satellites: If you want to be realistic, you should incorporate the nodal precession due to the Earth's oblateness into your analysis,

\frac{\dot \Omega}{\dot m} =<br /> -\,\frac 3 2 J_2 \left(\frac{R_E}{a}\right)^2 \cos i

where
  • \dot \Omega is the satellite's nodal precession rate,
  • \dot m = \surd(\mu_E/a^3) is the satellite's mean motion,
  • a is the satellite's semi-major axis,
  • i is the satellite's inclination,
  • J_2=0.00108263 is the Earth's dynamic oblateness,
  • \mu_E is the Earth's gravitational coefficient,
  • R_E is the Earth's equatorial radius.
 
Thanks for you replies DH.

I plugged in an altitude of 700 km and inclination of 98 deg into the expression you provided, and got a nodal precession rate of 0.963 degs/day.

I read that this is the rate of change of right ascension of the ascending node, which in this case would (almost) imply a fixed orbit plane with respect to the Earth-Sun vector (i.e. a sun-sync orbit). Is this equivalent with saying that the duration of the eclipse period for such an orbit is constant over the course of a year?

Also, are there any good free visualization tools out there one could use to get a better feel for how different orbits behave etc?
 
gnurf said:
Is this equivalent with saying that the duration of the eclipse period for such an orbit is constant over the course of a year?
That would be correct if the Earth's orbit about the Sun was circular. It isn't. For sun-synchronous satellites that fly roughly over local noon / local midnight, the effect is small. For those that fly roughly over the terminator, the effect is quite significant. These satellites can see the Sun all of the time for most of the year, but have a short eclipse season where the Sun is eclipsed by the Earth for part(s) of each orbit.

Also, are there any good free visualization tools out there one could use to get a better feel for how different orbits behave etc?
STK does a good job, and the basic version is free. I don't know what the basic version's capabilities are. (A useful, non-basic is far from free. STK makes Matlab look cheap.)
 

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