ConstantID

Shielded proton magnetic moment

Atomic & nuclearMeasured

μp′ = 1.410 570 5830(58) × 10−26 J T−1

Value
1.410 570 5830 × 10−26 J T−1
Standard uncertainty
5.8 × 10−35 J T−1
Relative uncertainty
4.1 × 10−9 (4.1 parts per billion)
Status
Measured
Symbol
μp′
Source
CODATA 2022 via NIST · NIST entry

Use in a calculation

# shielded proton magnetic moment, CODATA 2022 (NIST)
shielded_proton_magnetic_moment = 1.410570583e-26  # J T^-1, standard uncertainty 5.8e-35

# SciPy: scipy.constants.physical_constants['shielded proton mag. mom.']

What it is

The magnetic moment of a proton in a spherical sample of pure water at 25 °C, whose magnetic field is partly screened by the surrounding electrons: how strongly it behaves like a tiny bar magnet. A negative value means it points opposite to the spin.

How the value changed, 1998–2022

Each point is one CODATA adjustment, plotted as its difference from the 2022 value; the bars show one standard uncertainty (an arrowhead means the bar runs off the chart).

shielded proton magnetic moment: CODATA values 1998–2022 relative to the 2022 value, in parts per billion, with one-standard-uncertainty bars−200−1000+100+200parts per billion1998200220062010201420182022

Relative uncertainty

shielded proton magnetic moment: relative standard uncertainty in each CODATA adjustment, logarithmic scale10⁻⁹10⁻⁸10⁻⁷1998200220062010201420182022
CODATAValue (uncertainty)Relative uncertaintyChange from previous
20221.410 570 5830(58) × 10−264.1 × 10−9 +1.5 σ of 2018
20181.410 570 560(15) × 10−261.1 × 10−8 +0.7 σ of 2014
20141.410 570 547(18) × 10−261.3 × 10−8 +1.4 σ of 2010
20101.410 570 499(35) × 10−262.5 × 10−8 +2.1 σ of 2006
20061.410 570 419(38) × 10−262.7 × 10−8 −0.4 σ of 2002
20021.410 570 47(12) × 10−268.5 × 10−8 +1.2 σ of 1998
19981.410 570 399(59) × 10−264.2 × 10−8

“Change from previous” is the shift in the value divided by the standard uncertainty of the previous adjustment. Earlier values are converted into the current unit where NIST changed it (for example J s to J Hz⁻¹).

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