6.1.1 The Earth–Moon System
1. Earth’s motions – the reference frame for the Moon
- Rotation (day‑night cycle) – Earth rotates eastward once every ≈ 24 h (23 h 56 min sidereal). This gives the daily rise and set of the Sun and Moon.
- Axial tilt – The rotation axis is inclined ≈ 23.5° to the ecliptic plane. Combined with the yearly orbit it produces the seasons (AO1 1.2).
- Orbit around the Sun (year) – One complete revolution takes ≈ 365.25 days. The Earth travels roughly 30 km s⁻¹ at an average distance of 1 AU ≈ 1.5 × 10⁸ km.
2. Moon’s orbital periods
| Period | Definition | Typical value | How it is measured |
|---|
| Sidereal month | Time for the Moon to complete one full orbit relative to the distant stars | 27.32 days (≈ 655 h) | Star‑tracking observations |
| Synodic month | Time between two identical phases (e.g. New → New) | 29.53 days (≈ 709 h) | Phase‑cycle observations |
Why the two periods differ (AO1 6.1.1):
- During one sidereal orbit the Earth moves ≈ 30° (≈ 1° day⁻¹) around the Sun.
- To line up again with the Sun‑Earth direction, the Moon must travel an extra ≈ 30° in its orbit.
- Extra angular distance ≈ 30° ÷ (12.2° day⁻¹) ≈ 2.5 days, giving the longer synodic month.
3. Phase angle θ and the periodic nature of the lunar phases
The phase angle θ is the Sun–Earth–Moon angle measured at the centre of the Earth (Figure 1). As the Moon orbits, θ increases almost uniformly.
θ = ω t where ω = \(\displaystyle\frac{2\pi}{T{\rm syn}}\) and \(T{\rm syn}=29.53\) days.
Thus ω ≈ 2π / 29.53 ≈ 0.213 rad day⁻¹ ≈ 12.2° day⁻¹.
Because ω is essentially constant, after every synodic month the phase angle returns to the same value and the same lunar phase repeats – the cycle is periodic (AO2 6.1.1).
4. Sequence of lunar phases
| Phase | Relative Sun‑Moon‑Earth geometry | Phase angle θ | Illuminated fraction |
|---|
| New Moon | Moon between Sun and Earth | 0° (or 360°) | ≈ 0 % |
| Waxing Crescent | Moon moves eastward; Sun‑Moon line < 90° | 0° → 90° | 0 % → ≈ 50 % |
| First Quarter | Moon 90° east of the Sun | ≈ 90° | ≈ 50 % |
| Waxing Gibbous | Sun‑Moon angle 90° → 180° | 90° → 180° | ≈ 50 % → 100 % |
| Full Moon | Earth between Sun and Moon | ≈ 180° | ≈ 100 % |
| Waning Gibbous | Sun‑Moon angle 180° → 270° | 180° → 270° | 100 % → ≈ 50 % |
| Last (Third) Quarter | Moon 90° west of the Sun | ≈ 270° | ≈ 50 % |
| Waning Crescent | Sun‑Moon angle 270° → 360° | 270° → 360° | ≈ 50 % → 0 % |
5. Linking the orbital period to the phase cycle
- Average orbital speed of the Moon:
\(v = \dfrac{2\pi r}{T{\rm sid}}\) with \(r≈384 400\) km and \(T{\rm sid}=27.32\) days → \(v≈1.02\) km s⁻¹.
- Angular displacement per day: \(360°/29.53 ≈ 12.2°\) day⁻¹.
- Earth also moves ≈ 1° day⁻¹ around the Sun, so the Sun‑Earth line rotates slowly. The net change in the Sun‑Moon angle each day is therefore ≈ 12.2° (the Moon’s motion dominates).
- After one synodic month (≈ 29.5 days) the Moon has again the same angle θ relative to the Sun, so the same phase reappears – the phase cycle is periodic.
6. Why the Moon rises ≈ 50 minutes later each night
7. Common misconceptions (AO1 6.1.1)
- Moonlight comes from Earth – The illuminated side of the Moon is lit directly by sunlight. “Earth‑shine” is a faint glow on a thin crescent when sunlight reflected from Earth reaches the Moon’s dark side.
- The Moon rises at the same time each night – Because the Moon advances ≈ 12.2° eastward each day, it appears about 50 minutes later each successive night.
- Phases repeat every 27 days – The sidereal month (27.3 days) is the time to return to the same position against the stars. Identical phases repeat after the synodic month (≈ 29.5 days).
- The Moon is a source of its own light – The Moon has no intrinsic luminosity; it only reflects sunlight.
8. Suggested diagram (for classroom use)
A side‑view sketch showing the Sun, Earth and Moon at the eight principal phases. Include:
- Arrows indicating the direction of the Moon’s orbital motion (eastward).
- The Sun‑Earth line and the phase angle θ labelled for each phase.
- Relative positions of Earth’s shadow (for completeness, not required for phases).
9. Quick‑check questions (AO2 6.1.1)
- State the lengths of the sidereal and synodic months and explain why they differ.
- Calculate the angular speed ω of the Moon in degrees per day and use it to find the phase angle after 7 days from a New Moon.
- Explain why the Moon rises later each night and show the calculation that gives ≈ 50 minutes.
- If the Moon were stationary relative to Earth, what would an observer on Earth see each night?
- Describe Earth‑shine and indicate when it can be observed.
10. Key constants and formulas (AO1 6.1.1)
| Quantity | Symbol | Value | Notes |
|---|
| Earth rotation period (solar day) | 24 h | ≈ 86 400 s |
| Earth orbital period | 1 yr | ≈ 365.25 days |
| Mean Earth‑Sun distance (1 AU) | rES | 1.496 × 10⁸ km |
| Mean Moon‑Earth distance | rEM | 3.844 × 10⁵ km |
| Sidereal month | Tsid | 27.32 days |
| Synodic month | Tsyn | 29.53 days |
| Moon’s average orbital speed | v | ≈ 1.02 km s⁻¹ | \(v=2\pi r/T_{\rm sid}\) |
| Angular speed of phase change | ω | ≈ 12.2° day⁻¹ | \(ω=360°/T_{\rm syn}\) |