ConstantID

Shielded proton gyromagnetic ratio

Atomic & nuclearMeasured

γp′ = 2.675 153 194(11) × 108 s−1 T−1

Value
2.675 153 194 × 108 s−1 T−1
Standard uncertainty
1.1 s−1 T−1
Relative uncertainty
4.1 × 10−9 (4.1 parts per billion)
Status
Measured
Symbol
γp′
Source
CODATA 2022 via NIST · NIST entry

Use in a calculation

# shielded proton gyromagnetic ratio, CODATA 2022 (NIST)
shielded_proton_gyromagnetic_ratio = 2.675153194e8  # s^-1 T^-1, standard uncertainty 1.1

# SciPy: scipy.constants.physical_constants['shielded proton gyromag. ratio']

What it is

The ratio of magnetic moment to angular momentum for a proton in a spherical sample of pure water at 25 °C, whose magnetic field is partly screened by the surrounding electrons. In a magnetic field B the spin precesses at angular frequency γB; this is the basis of magnetic resonance.

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 gyromagnetic ratio: CODATA values 1998–2022 relative to the 2022 value, in parts per billion, with one-standard-uncertainty bars−150−100−500+50+100+150parts per billion1998200220062010201420182022

Relative uncertainty

shielded proton gyromagnetic ratio: relative standard uncertainty in each CODATA adjustment, logarithmic scale10⁻⁹10⁻⁸10⁻⁷1998200220062010201420182022
CODATAValue (uncertainty)Relative uncertaintyChange from previous
20222.675 153 194(11) × 1084.1 × 10−9 +1.5 σ of 2018
20182.675 153 151(29) × 1081.1 × 10−8 −0.6 σ of 2014
20142.675 153 171(33) × 1081.2 × 10−8 −1.5 σ of 2010
20102.675 153 268(66) × 1082.5 × 10−8 −1.3 σ of 2006
20062.675 153 362(73) × 1082.7 × 10−8 +0.1 σ of 2002
20022.675 153 33(23) × 1088.6 × 10−8 −0.7 σ of 1998
19982.675 153 41(11) × 1084.1 × 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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