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Solar-Mass Geometric Conversions

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Solar-mass geometric units turn a dimensionless relativistic calculation into lengths, times, and frequencies without first assigning the Sun a mass in kilograms. The safe input is the mass parameter GMGM: astronomical dynamics usually determines this product more directly than either factor separately. This card uses an exact nominal solar conversion in the denominator and keeps the chosen physical mass, frequency convention, and reference frame explicit.

The International Astronomical Union defines the nominal solar mass parameter

(GM)⊙N=1.3271244×1020 m3 s−2(GM)_\odot^{\mathrm N}=1.3271244\times10^{20}\ \mathrm{m^3\,s^{-2}}

as an exact conversion constant, not as a measurement of the present Sun IAU 2015, Resolution B3, Recommendations 1–4 and solar conversion table, printed pp. 1–2, PDF. For a chosen system mass parameter GMGM, define on this card

M≡GM(GM)⊙N.\mathcal M\equiv\frac{GM}{(GM)_\odot^{\mathrm N}}.

Thus M\mathcal M is a dimensionless scaling ratio. It inherits any uncertainty in the inferred numerator; the nominal denominator contributes none. Here M\mathcal M does not automatically mean the binary chirp mass, despite the common use of the same calligraphic letter for that different quantity.

Exact geometric units per nominal solar mass

Section titled “Exact geometric units per nominal solar mass”

The SI speed of light is exactly c=299 792 458 m s−1c=299\,792\,458\ \mathrm{m\,s^{-1}} BIPM 2026, SI Brochure, §2.2, Table 1, printed p. 124, PDF. Combining two exact conversion constants gives

rg,⊙N≡(GM)⊙Nc2,tg,⊙N≡(GM)⊙Nc3,rs,⊙N≡2rg,⊙N.\begin{aligned} r_{g,\odot}^{\mathrm N} &\equiv\frac{(GM)_\odot^{\mathrm N}}{c^2}, &t_{g,\odot}^{\mathrm N} &\equiv\frac{(GM)_\odot^{\mathrm N}}{c^3},\\ r_{s,\odot}^{\mathrm N} &\equiv 2r_{g,\odot}^{\mathrm N}. \end{aligned}
ConversionRounded decimal display
rg,⊙Nr_{g,\odot}^{\mathrm N}1.476625038… km1.476625038\ldots\ \mathrm{km}
tg,⊙Nt_{g,\odot}^{\mathrm N}4.925490948… μs4.925490948\ldots\ \mathrm{\mu s}
rs,⊙Nr_{s,\odot}^{\mathrm N}2.953250076… km2.953250076\ldots\ \mathrm{km}

The formulas, rather than the displayed decimals, are exact. The ellipses mark rounding of nonterminating decimal expansions; they are not experimental error bars. The identities ctg,⊙N=rg,⊙Nct_{g,\odot}^{\mathrm N}=r_{g,\odot}^{\mathrm N} and rs,⊙N=2rg,⊙Nr_{s,\odot}^{\mathrm N}=2r_{g,\odot}^{\mathrm N} provide immediate unit and normalization checks.

Suppose a calculation uses GM/c2GM/c^2 as its length unit and GM/c3GM/c^3 as its time unit. If L^\widehat L, t^\widehat t, and ω^\widehat\omega are defined by

L^=Lc2GM,t^=tc3GM,ω^=ωGMc3,\widehat L=\frac{Lc^2}{GM},\qquad \widehat t=\frac{tc^3}{GM},\qquad \widehat\omega=\frac{\omega GM}{c^3},

then the physical quantities are

L=L^ Mrg,⊙N,t=t^ Mtg,⊙N,ω=ω^Mtg,⊙N,f=ω^2πMtg,⊙N.\begin{aligned} L&=\widehat L\,\mathcal M r_{g,\odot}^{\mathrm N}, &t&=\widehat t\,\mathcal M t_{g,\odot}^{\mathrm N},\\ \omega&=\frac{\widehat\omega} {\mathcal M t_{g,\odot}^{\mathrm N}}, &f&=\frac{\widehat\omega} {2\pi\mathcal M t_{g,\odot}^{\mathrm N}}. \end{aligned}

Numerically, with the exact nominal inputs rounded only for display,

L=(1.476625038… km) ML^,t=(4.925490948… μs) Mt^,ω=(2.030254467…×105 s−1)ω^M,f=(3.231250342…×104 Hz)ω^M.\begin{aligned} L&=(1.476625038\ldots\ \mathrm{km})\,\mathcal M\widehat L,\\ t&=(4.925490948\ldots\ \mathrm{\mu s})\,\mathcal M\widehat t,\\ \omega&=(2.030254467\ldots\times10^5\ \mathrm{s^{-1}}) \frac{\widehat\omega}{\mathcal M},\\ f&=(3.231250342\ldots\times10^4\ \mathrm{Hz}) \frac{\widehat\omega}{\mathcal M}. \end{aligned}

The last line assumes the code reports dimensionless angular frequency ω^\widehat\omega. If it instead reports f^=fGM/c3\widehat f=fGM/c^3, then f=f^/(Mtg,⊙N)f=\widehat f/(\mathcal M t_{g,\odot}^{\mathrm N}) with no additional 2π2\pi. The same time map converts waveform timestamps, damping times, and orbital periods once their normalization is declared.

The first trap is the factor of two. The geometric mass length is rg=GM/c2r_g=GM/c^2, whereas the Schwarzschild horizon radius is rs=2GM/c2r_s=2GM/c^2. A code statement such as “r=2Mr=2M” normally uses M=rgM=r_g; replacing that MM by a quoted Schwarzschild radius doubles the answer again. For rotating black holes, neither 2rg2r_g nor the Boyer–Lindquist coordinate r+r_+ should be treated as a universal invariant size; use the convention- controlled Black-Hole Horizon Scales record.

The second trap is 2π2\pi. Angular frequency obeys ω=2πf\omega=2\pi f. Before using a tabulated prefactor, inspect both the symbol and the defining equation: a number labeled merely “frequency” does not reveal whether it is in s−1\mathrm{s^{-1}} or cycles per second. The broader restoration rules are in Units and Dimensional Conventions, and the standards inputs are collected in Fundamental Constants Used in Gravity.

Converting the exact nominal parameter to kilograms requires a measured value of GG. Using the 2022 CODATA recommendation G=6.67430(15)×10−11 m3 kg−1 s−2G=6.67430(15)\times10^{-11}\ \mathrm{m^3\,kg^{-1}\,s^{-2}} Mohr et al. 2025, Table XXXIII, p. 025002-45, NIST-hosted PDF gives

(GM)⊙NG=1.988410(45)×1030 kg.\frac{(GM)_\odot^{\mathrm N}}{G} =1.988410(45)\times10^{30}\ \mathrm{kg}.

The relative standard uncertainty is that of GG, about 2.25×10−52.25\times10^{-5} or 22.522.5 parts per million. This kilogram value is therefore measured-model dependent; it is not another exact nominal constant, and changing the adopted GG changes it.

Finally, the conversion does not decide which mass belongs in GMGM. A binary calculation may use total mass, a component mass, chirp mass, or final remnant mass, while a perturbation calculation may normalize by the background mass. Source-frame and detector-frame masses differ when cosmological redshift is relevant, so the mass frame must match the frame of the reported time or frequency. If a detector-frame mass scales a detector-frame waveform, do not apply the redshift factor a second time. Object inference and the meanings of astrophysical mass parameters belong to Identifying Astrophysical Black Holes.

  • Bureau International des Poids et Mesures. The International System of Units (SI). 9th ed., version 4.01. Sèvres: BIPM, 2026. DOI. Official PDF.
  • International Astronomical Union. “Resolution B3 on Recommended Nominal Conversion Constants for Selected Solar and Planetary Properties.” XXIX General Assembly, 2015. Official PDF.
  • Mohr, Peter J., David B. Newell, Barry N. Taylor, and Eite Tiesinga. “CODATA Recommended Values of the Fundamental Physical Constants: 2022.” Reviews of Modern Physics 97 (2025): 025002. DOI. NIST-hosted PDF.