This post is the companion to the short film Has Stonehenge drifted off its line? Stonehenge was laid out on the solstice axis about 2500 BC. Three slow movements could have shifted that line since: the wobble of the Earth's axis, the easing of its tilt, and the drift of the ground itself. Only one of them has moved the solstice sunrise by a measurable amount. The numbers, methods and caveats follow.
The question
The main axis of Stonehenge runs from the midsummer sunrise in the north-east to the midwinter sunset in the south-west, at 49.95° true (49.81° on the National Grid; Thom et al. 1974). The sarsen structure is taken here as built about 2500 BC. The question is whether anything has since moved the line between the stones and the Sun.
Stonehenge in 2500 BC (red) and today, about 100 m to the north-east. The two axes are parallel. Plan from T. Daw's 3D model.
1. Precession: the stars change, the sunrise does not
The Earth's axis wobbles like a spinning top, tracing a cone about once in 25,800 years. The north pole of the sky moves with it. Thuban, in Draco, "passed within 0.1° of the pole in 2800 BC" (Rawlins & Pickering 2001); today the pole lies near Polaris. Using the long-term precession model of Vondrák, Capitaine & Wallace (2011) and Thuban's J2000 position (proper motion ignored), the closest approach comes out at 0.05° in 2791 BC, consistent with that figure.
Precession changes which stars stand behind the Sun at the solstice, and the calendar date of the solstice. It does not change where the solstice Sun rises. At a solstice the Sun's declination equals the obliquity, plus or minus, and the rising azimuth depends only on declination, latitude, the altitude of the horizon and refraction (Meeus 1998; Ruggles 1999).
The path of the north pole of the sky from 2800 BC to 2026 (gold), on its 25,800-year circle (dotted). Vondrák et al. 2011.
2. The tilt: the sunrise has moved about one degree
The obliquity, the tilt of the Earth's axis to its orbit, has fallen from 23.973° in 2500 BC to 23.436° today (Vondrák et al. 2011, through the ERFA library; Laskar 1986 gives 23.974° for 2500 BC). That is a change of 0.537°. Taking 2700 BC or 2300 BC instead gives 23.992° or 23.954°.
Where the Sun appears on the skyline also depends on how high the skyline is. The horizon was computed from the Environment Agency's 1 m LiDAR terrain model (5 m beyond 2 km), from the centre of the circle (51.1789° N, 1.8262° W) with the eye 1.5 m above the ground, allowing for the curvature of the Earth and terrestrial refraction. Stones and trees are ignored. To the north-east the skyline is a ridge about 2.7 km away, 0.57° high at the 2500 BC sunrise and 0.60° at today's. To the south-west it lies about 4.3 km away, at 0.46–0.49°.
With Bennett's (1982) formula for refraction and a solar semi-diameter of 0.267°:
- Midsummer sunrise, first gleam: 49.33° in 2500 BC, 50.42° today, a shift of 1.09°. With the half disc showing, 49.79° to 50.86°; with the whole disc risen, 50.25° to 51.30°.
- Midwinter sunset, last gleam: 230.02° in 2500 BC, 231.08° today, a shift of 1.06°.
The Sun is 0.53° across, so the sunrise has moved about two widths of the Sun. Moving the date of construction 200 years either way changes these azimuths by less than 0.05°. Refraction near the horizon varies with the weather by a few tenths of a degree; that moves both dates alike and leaves the shift unchanged.
The north-east skyline from the centre of Stonehenge, from Environment Agency LiDAR, with the first gleam of the midsummer Sun in 2500 BC and 2026. Vertical and horizontal scales equal.
3. The ground: Rujm el-Hiri
The third movement is the ground itself. Rujm el-Hiri is a large stone ring in the Golan Heights, about 150 m across, with a central cairn. Aveni & Mizrachi (1998) proposed that its layout held solstice and other sky alignments. Khabarova, Birkenfeld & Eppelbaum (2024) argued from geomagnetic evidence that the whole region has rotated, and that this undermines the observatory interpretation. Their figure (section 3):
"Assuming the average rotation velocity of 10 mm per year and the age of the studied prehistoric site as 4000 years, we will receive an arc rotation of about 40 m. The corresponding direct movement can be estimated as 30 m to its today's position."
The paper gives a distance. It gives no angle through which the site has turned.
The Sea of Galilee and Rujm el-Hiri. Lake outline: Natural Earth.
The rings of Rujm el-Hiri (schematic) and the paper's 30 m shift, drawn to the same scale.
A shift is not a turn
The Sun is so far away that its light arrives in parallel lines. Sliding a monument sideways, by 30 m or 30 km, leaves every bearing within it unchanged: a line that pointed at the solstice sunrise still does. To spoil a solar alignment, the ground has to turn, and by something like the width of the Sun, about 0.5°.
No rotation angle is published for Rujm el-Hiri. As an order of magnitude only: fast block rotations measured from palaeomagnetism run at 1–20° per million years, which over 4,500 years gives 0.005–0.09°. That is well short of a Sun-width. This bound is ours, not the paper's.
Diagram: a monument slid sideways still points at sunrise; turned, it does not. Movement and angles exaggerated.
Stonehenge on the Eurasian plate
Stonehenge sits on the Eurasian plate, which rotates slowly about a pole in North America. Evaluating the plate's rotation at the monument:
- ITRF2014 plate motion model (Altamimi et al. 2017; Eurasia ω = −0.085, −0.531, 0.770 mas a year): 16.5 mm a year north and 16.5 mm a year east, so 23.4 mm a year on a bearing of 045°. Over the 4,525 years since 2500 BC that is 106 m: 75 m north and 75 m east.
- NNR-MORVEL56 (Argus, Gordon & DeMets 2011; pole 48.85° N, 106.50° W, 0.223 ± 0.009° per million years): 21.7 mm a year on 043°, 98 m since 2500 BC.
These speeds are measured against the average motion of all the plates (the no-net-rotation frame), which is a convention. Relative to Africa or North America the figures differ; the rotation of the ground under Stonehenge, which is what matters for an alignment, does not depend on the frame chosen.
The Eurasian plate (shaded) and its boundaries, PB2002 (Bird 2003), with Stonehenge's motion. Inset: the monument's 106 m since 2500 BC, to scale.
Has Stonehenge turned?
The component of the plate's rotation about the local vertical at Stonehenge is 2.5 arcseconds anticlockwise since 2500 BC (ITRF2014; 1.8 arcseconds with NNR-MORVEL56), or 0.0007°. Moving 75 m north also raises the latitude by 0.00067°, which moves the solstice sunrise by 2.5 arcseconds, also anticlockwise. The monument and the sunrise have turned the same way by the same amount, so the alignment between them has changed by well under an arcsecond.
A larger term is polar motion: the slow drift of the spin axis relative to the whole crust. At today's secular rate of about 3.5–4 milliarcseconds a year, much of it from rebound after the last ice age and not necessarily constant over 4,500 years, it amounts to roughly 16–18 arcseconds of pole shift, of order 0.005°.
Taking everything together, the ground under Stonehenge has turned by less than a hundredth of a degree against the sky. The easing of the tilt has moved the solstice sunrise about a hundred times further. Stonehenge has moved about 100 m, but its solstice line has not turned.
Change in the solstice sunrise since 2500 BC: precession 0°, tilt about 1°, drift under 0.01°.
Corrections to the 2025 post
The post of 8 January 2025, "The tectonic movement of Stonehenge", reached the right conclusion: continental drift has not changed Stonehenge's solstice alignment by any measurable amount. Four of its figures need correcting:
- "approximately 25 millimeters per year": about 22–23 mm a year (21.7–23.4 mm, depending on the model). "About 2 cm a year" stands.
- "125 meters northward" in 5,000 years: about 100 m north-east since 2500 BC, of which about 75 m is northward. Over a full 5,000 years the total would be about 115 m.
- "rotating clockwise": the Eurasian plate rotates anticlockwise about its pole in North America; at Stonehenge, about 2.5 arcseconds anticlockwise since 2500 BC.
- "one-thousandth of a degree of latitude": 0.00067°.
Notes on the film
Every number in the film was computed for it from open data, with the scripts in the film's folder: the horizon from Environment Agency LiDAR, the Sun's positions with the ERFA implementation of Vondrák et al. (2011), the plate motion from the published rotation poles, and the path of the celestial pole. Published horizon profiles were used only as a cross-check. The plan of Stonehenge is from T. Daw's 3D model; the rings of Rujm el-Hiri are a schematic; maps use Natural Earth and the PB2002 plate boundaries. The film quotes only the 2024 paper's own figures for Rujm el-Hiri. Music: original.
Sources
- Altamimi, Z., Métivier, L., Rebischung, P., Rouby, H. & Collilieux, X. 2017. ITRF2014 plate motion model. Geophysical Journal International 209, 1906–1912. doi:10.1093/gji/ggx136
- Argus, D. F., Gordon, R. G. & DeMets, C. 2011. Geologically current motion of 56 plates relative to the no-net-rotation reference frame. Geochemistry, Geophysics, Geosystems 12, Q11001. doi:10.1029/2011GC003751
- Aveni, A. & Mizrachi, Y. 1998. The geometry and astronomy of Rujm el-Hiri, a megalithic site in the southern Levant. Journal of Field Archaeology 25, 475–496. doi:10.1179/009346998792005261
- Bennett, G. G. 1982. The calculation of astronomical refraction in marine navigation. Journal of Navigation 35, 255–259. doi:10.1017/S0373463300022037
- Bird, P. 2003. An updated digital model of plate boundaries. Geochemistry, Geophysics, Geosystems 4, 1027. doi:10.1029/2001GC000252
- Daw, T. 2025. The tectonic movement of Stonehenge. sarsen.org, 8 January 2025.
- Environment Agency 2022. LIDAR Composite DTM 1 m. Contains Environment Agency data. © Environment Agency copyright and/or database right 2022. Open Government Licence v3.0.
- Khabarova, O., Birkenfeld, M. & Eppelbaum, L. V. 2024. Discussion points of the remote sensing study and integrated analysis of the archaeological landscape of Rujm el-Hiri. Remote Sensing 16, 4239. doi:10.3390/rs16224239
- Laskar, J. 1986. Secular terms of classical planetary theories using the results of general relativity. Astronomy & Astrophysics 157, 59–70.
- Meeus, J. 1998. Astronomical Algorithms, 2nd edn. Willmann-Bell.
- Rawlins, D. & Pickering, K. 2001. Astronomical orientation of the pyramids. Nature 412, 699. doi:10.1038/35089138
- Ruggles, C. 1999. Astronomy in Prehistoric Britain and Ireland. Yale University Press.
- Thom, A. et al. 1974. Stonehenge. Journal for the History of Astronomy 5, 71–90.
- Vondrák, J., Capitaine, N. & Wallace, P. 2011. New precession expressions, valid for long time intervals. Astronomy & Astrophysics 534, A22. doi:10.1051/0004-6361/201117274



















