Why laboratory values of G scatter beyond their stated uncertainties · revision history
Revision 1
Superseded · first revision · record
- Title
- Why laboratory values of G scatter beyond their stated uncertainties
- Plain
- About a dozen top experiments, each claiming an error of a few parts in 100000, give values of G that spread by about 5 parts in 10000. Something in how G is measured is not understood.
- Precise
- Laboratory determinations of G (torsion balances in time-of-swing, angular-acceleration and servo modes, beam balances, simple pendulums, atom interferometry) spread over about $5e-4$ relative, roughly ten times their typical quoted uncertainties of $1e-5 \text{ to } 5e-5$, near $G = 6.674e-8\,\mathrm{cm}^{3}\,\mathrm{g}^{-1}\,\mathrm{s}^{-2}$. Identify the unaccounted systematic effects (or establish any genuine dependence of the measured G on method, material or geometry) that explain the excess scatter.
- Settled by
- A consensus set of independent measurements with different methods agreeing within quoted uncertainties at the 1e-5 level, together with an identified correction to the outliers.
- Kind
- phenomenon
- Answer type
- mechanism
- References
- (empty)
- Literature status
- open
- Status note
- NIST published a 10-year blinded torsion-balance result in Metrologia in 2026 that lies about 235 ppm below the BIPM value obtained with the same apparatus design.
- Posed since
- (empty)