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Pole forecast Where the poles will be, and how uncertain that is

A forecast is only as good as the forecasts it could have made. Each method is replayed on the past: from every year from 1950 to 2024 it forecasts the pole 1 to 25 years later, and the distance to the actual position gives its typical error at each horizon. The forecast shown is that of the method that erred least, and its cone of uncertainty is that of its past errors: 50 % of cases inside the full circle, 90 % inside the dashed one. Observed positions: position of the poles; reversals: field reversal.
Speed of the north magnetic pole in 2025 (km/yr)
36.6
maximum of 58 km/yr in 2011: the pole is slowing down
Forecast displacement by 2030 (km)
175
towards 84.6° N, 124.9° E; 50 % radius: 26 km, 90 %: 66 km
Forecast displacement by 2050 (km)
731
towards 80.3° N, 104.7° E; 50 % radius: 270 km, 90 %: 661 km
Difference with WMM2025 in 2030 (km)
15
official NOAA/BGS forecast; poles computed here within 0.04 km of NOAA’s

Tracks and forecasts on the globe

The north pole has left Canada for Siberia; the south pole drifts slowly off Adélie Land. Turn the globe, hover a point for its year and position, tick the layers to show; the circles hold 50 % (light) and 90 % (pink) of the past errors of the retained method at that horizon.

Drag to turn · wheel to zoom · hover a point

North magnetic pole

Forecast shown (mean of the methods) from 2025, and spread between methods
YearPositionDisplacement50 % / 90 % radiusSpread of methods
203084.65°, 124.9°175 km26 / 66 km25 km
203583.52°, 116.7°331 km72 / 179 km69 km
204082.41°, 111.3°474 km129 / 319 km127 km
205080.32°, 104.7°731 km270 / 661 km303 km
Error of the replayed forecasts (median / 9 cases out of 10, km), and mean error at 5–20 years before and after 1990
Method5 yr10 yr20 yrbefore 1990after 1990
extrapolated field 27.9 / 64.883.1 / 187.1218.2 / 541.8 100.7183.7
mean of the methods 26.6 / 58.868.7 / 163.5205.5 / 524.8 106.5132.2
constant velocity 24.6 / 64.160.4 / 188.8179.3 / 548.4 94.1154.8
extrapolated field with acceleration 30 / 56.891.2 / 153.1268.5 / 538.1 153.8127.1
constant acceleration 45.1 / 86.7105.6 / 218.2278.5 / 626.3 130248.6

In 2030, the official WMM2025 forecast is 15 km from this one.

South magnetic pole

Forecast shown (constant velocity) from 2025, and spread between methods
YearPositionDisplacement50 % / 90 % radiusSpread of methods
2030-63.63°, 134.3°46 km9 / 32 km4 km
2035-63.40°, 133.5°92 km23 / 80 km12 km
2040-63.17°, 132.7°139 km40 / 136 km23 km
2050-62.69°, 131.2°231 km81 / 267 km58 km
Error of the replayed forecasts (median / 9 cases out of 10, km), and mean error at 5–20 years before and after 1990
Method5 yr10 yr20 yrbefore 1990after 1990
extrapolated field 8.7 / 34.822.4 / 94.363 / 243.5 61.724.8
mean of the methods 8.4 / 28.420.7 / 73.866.5 / 316.2 65.420.1
constant velocity 8.7 / 2821.6 / 79.761.1 / 205 57.723.6
extrapolated field with acceleration 7.4 / 2822 / 120.3122.1 / 532.2 104.523.2
constant acceleration 12.7 / 66.434.6 / 151.3127.3 / 482 128.325.8

In 2030, the official WMM2025 forecast is 2.5 km from this one.

Speed of the magnetic poles since 1900
Show the data as a table
Error of the forecasts by horizon (north pole)
Show the data as a table

Dipole axis and magnetic moment

The dip pole (where the compass points down) follows the irregularities of the field near the pole; the dipole axis, the simplest part of the field, moves far more slowly: its boreal pole is in 2025 at 80.8° N, -72.8° E. The dipole moment went from 8.32 to 7.69 × 10²² A·m² between 1900 and 2025, i.e. -6.4 % per century (-6.3 % per century over the last 50 years). Extending this decline to zero makes no physical sense: the moment has varied like this before without reversing, and no model forecasts a reversal.

Moment of the Earth’s magnetic dipole since 1900
Show the data as a table

The rotation pole

The Earth’s rotation axis also moves relative to the crust, but by a few centimetres a year: since 2000 its mean pole has drifted by 13.5 ± 2.1 cm/yr towards 14° W (± 9°), driven by melting ice and water moving on the continents (Adhikari & Ivins, 2016; Deng et al., 2021). Measurements and fit: position of the poles. If this drift continued:

  • 2050: about 3.2 m (± 1.0 m) from today
  • 2100: about 10.0 m (± 3.1 m) from today
Method and sources

Poles. For every year since 1900, the dip pole (point where the horizontal component of the field vanishes) is computed from the Gauss coefficients of IGRF-14 (Alken et al., 2021), at sea level on the WGS84 ellipsoid, by Newton iterations; it differs from the one published by NOAA by a few hundredths of a kilometre in median.

Methods. Each uses only what was known in the starting year. Constant velocity: that of the last 5 years, along the great circle. Constant acceleration: parabola fitted over 15 years. Extrapolated field: Gauss coefficients extended with their change over the last 5 years, as the predictive part of IGRF and WMM, then the pole of the extended field. Field with acceleration: the change of the change over 10 years is added. Mean: average position of the velocity, field and field-with-acceleration methods.

Judging. Forecasts replayed from every year from 1950 to 2024, 1–25 years ahead; error = great-circle distance to the actual position. Method shown: smallest mean error at 5–20 years over all starting years (the ranking before and after 1990 is given to judge its stability). Cone: 50 % and 90 % quantiles of its past errors, fitted as a power law of the horizon.

Reading these data
The magnetic pole moves because liquid iron moves in the core: its accelerations (that of the 1990s, ascribed to magnetic flux expulsion under Canada and the elongation of a lobe under Siberia: Chulliat et al., 2010; Livermore et al., 2020) give no warning in surface measurements. The cones come from the last 75 years: a change of regime larger than any seen since would fall outside the 90 % cone. The dip pole is a landmark of the field, not an object: it can split or jump if the field changes shape. Before 1900 positions come from historical models (GUFM1), less precise, hence the trials starting in 1950. Errors from neighbouring start years are not independent (their windows overlap): the 75 hindcasts are worth far fewer than 75 trials, and at 25 years only the start years 1950–2000 count. Between its 5-year epochs the IGRF varies linearly: the yearly speed of the pole changes in steps at round years, an effect of the model, not of the core.
SOURCES OF THIS PAGE
Alken et al. (2021)
Alken, P., Thébault, E., Beggan, C. D., Amit, H., Aubert, J., et al. (2021). International Geomagnetic Reference Field: the thirteenth generation. Earth, Planets and Space, 73, 49. · doi:10.1186/s40623-020-01288-x
Licence : Published literature; cited
Livermore et al. (2020)
Livermore, P. W., Finlay, C. C., & Bayliff, M. (2020). Recent north magnetic pole acceleration towards Siberia caused by flux lobe elongation. Nature Geoscience, 13(5), 387–391. · doi:10.1038/s41561-020-0570-9
Licence : Published literature; cited
Chulliat et al. (2010)
Chulliat, A., Hulot, G., & Newitt, L. R. (2010). Magnetic flux expulsion from the core as a possible cause of the unusually large acceleration of the north magnetic pole during the 1990s. Journal of Geophysical Research, 115, B07101. · doi:10.1029/2009JB007143
Licence : Published literature; cited
Jackson et al. (2000)
Jackson, A., Jonkers, A. R. T., & Walker, M. R. (2000). Four centuries of geomagnetic secular variation from historical records. Philosophical Transactions of the Royal Society A, 358(1768), 957–990. · doi:10.1098/rsta.2000.0569
Licence : Published literature; cited
Adhikari et al. (2016)
Adhikari, S., & Ivins, E. R. (2016). Climate-driven polar motion: 2003–2015. Science Advances, 2(4), e1501693. · doi:10.1126/sciadv.1501693
Licence : Published literature; cited
Deng et al. (2021)
Deng, S., Liu, S., Mo, X., Jiang, L., & Bauer-Gottwein, P. (2021). Polar drift in the 1990s explained by terrestrial water storage changes. Geophysical Research Letters, 48(7), e2020GL092114. · doi:10.1029/2020GL092114
Licence : Published literature; cited
IERS Bulletin A daily Earth orientation (USNO finals2000A.all)
IERS Rapid Service/Prediction Centre (USNO), Bulletin A: polar motion, UT1−UTC and length of day since 1973, with predictions (finals2000A.all). · source page ↗
Licence : U.S. Government work, public domain; cite IERS Bulletin A · retrieved on Oct 23, 2026 · SHA-256 95a61292c957…