Theory — The Moving Sky
To describe where things are and how they move, astronomers imagine the sky as a giant celestial sphere surrounding the Earth. Directions on it are given by two angles, much like latitude and longitude on the Earth. The sphere appears to turn once a day because the Earth rotates; the daily circles that stars trace are called their diurnal motion.
1. The celestial sphere
Key reference points: the celestial poles lie above the Earth’s poles, the celestial equator is the projection of the Earth’s equator, and the ecliptic is the Sun’s yearly path, tilted about 23.5 degrees to the equator. Your local horizon and meridian (the north–south line through the zenith) fix what is up at any moment. The seasons arise from that 23.5 degree tilt, not from any change in the Earth–Sun distance.
2. Kepler’s laws
First law: each planet moves on an ellipse with the Sun at one focus. Second law: a line from the Sun to the planet sweeps out equal areas in equal times, so a planet moves faster when it is closer to the Sun. Third law links period and size of the orbit:
So P = √(a3) and a = P(2/3)
Newton later showed this law follows from gravity, and in its full form it also depends on the mass of the central body, which is how the mass of a planet or star is measured from the orbit of a companion.
3. Phases of the Moon
The Moon shines by reflected sunlight, so exactly half of it is always lit. Which part of the lit half we see depends on the angle between the Sun, Earth, and Moon as the Moon orbits us once a month. When the Moon is between us and the Sun we see the unlit side (new Moon); when the Earth is between the Sun and Moon we see the fully lit side (full Moon); in between we see crescents, quarters, and gibbous phases.
4. Why eclipses are rare
If the Moon’s orbit lay exactly in the plane of the Earth’s orbit, we would get a solar eclipse at every new Moon and a lunar eclipse at every full Moon. But the Moon’s orbit is tilted about 5 degrees, so its shadow usually misses. Eclipses happen only when a new or full Moon occurs near a node, where the two orbit planes cross.
Apparatus
Positional astronomy uses instruments for modelling the sphere, tracking orbital motion, and reading the Sun and Moon. In the simulation these are modelled, but the readings match what each instrument would give.
Instructions
Work through both tabs. Record your values, and for each task calculate first by hand, then use the button to compare with the simulation.
Part A — Kepler’s third law
- Choose a planet and read its semi-major axis
ain AU. - Using
P = √(a3), calculate the orbital period in years by hand. - Enter your period and press Check. The simulation compares it with the accepted value within 3 percent.
- Repeat for a second planet, then solve one reverse case: given a period, find the semi-major axis.
Part B — Moon phases and eclipses
- Move the Moon around its orbit and watch the lit fraction change in the geometry view.
- Predict the phase name and whether an eclipse is possible at that position (near a node), then press Check.
Simulation
Team Questions
Example Report
Worked example: the period of Mars
Mars has a semi-major axis of a = 1.524 AU. Apply Kepler’s third law:
P = √(a3) = √(1.5243) = √(3.54) ≈ 1.88 years.
The accepted orbital period of Mars is 1.88 years, so the calculated and accepted values agree. Reading the semi-major axis from the orbit and predicting the period this way is the calculate-then-compare core of the lab.