Jupiter mass unit
data derived with UnitSystems.jl
\[\text{M}\]
\[\left[\text{m}_\text{e}\right]\]
| Quantity | Product | UnitSystem |
|---|---|---|
| $1.898124(42) \times 10^{27}$ $\left[\text{kg}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | Metric |
| $1.898124(42) \times 10^{27}$ $\left[\text{kg}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | SI2019 |
| $1.898124(42) \times 10^{27}$ $\left[\text{kg}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | SI1976 |
| $1.898124(42) \times 10^{27}$ $\left[\text{kg}\right]$ | $\hbar^{-2}\text{c}^{-1}\text{R}_\text{K}^{-1}\text{K}_\text{J}^{-2}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau\cdot 2^{2}$ | CODATA |
| $1.898124(42) \times 10^{27}$ $\left[\text{kg}\right]$ | $\hbar^{-2}\text{c}^{-1}{\text{R}_\text{K}^{90}}^{-1}{\text{K}_\text{J}^{90}}^{-2}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau\cdot 2^{2}$ | Conventional |
| $1.897811(42) \times 10^{27}$ $\left[\text{kg}\right]$ | $\hbar^{-1}\text{c}^{-1}\Omega_\text{it}\cdot \text{V}_\text{it}^{-2}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | International |
| $1.897763(42) \times 10^{27}$ $\left[\text{kg}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau/1.0001900224889804$ | InternationalMean |
| $1.898124(42) \times 10^{27}$ $\left[\text{kg}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | MetricTurn |
| $1.898124(42) \times 10^{27}$ $\left[\text{kg}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | MetricSpatian |
| $1.898124(42) \times 10^{27}$ $\left[\text{kg}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | MetricGradian |
| $1.898124(42) \times 10^{27}$ $\left[\text{kg}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | MetricDegree |
| $1.898124(42) \times 10^{27}$ $\left[\text{kg}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | MetricArcminute |
| $1.898124(42) \times 10^{27}$ $\left[\text{kg}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | MetricArcsecond |
| $1.898124(42) \times 10^{27}$ $\left[\text{kg}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | Engineering |
| $1.935548(43) \times 10^{26}$ $\left[\text{hyl}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{g}_0^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | Gravitational |
| $1.898124(42) \times 10^{24}$ $\left[\text{t}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau\cdot 2^{-3}5^{-3}$ | MTS |
| $1.898124(42) \times 10^{30}$ $\left[\text{g}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau\cdot 2^{3}5^{3}$ | EMU |
| $1.898124(42) \times 10^{30}$ $\left[\text{g}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau\cdot 2^{3}5^{3}$ | ESU |
| $1.898124(42) \times 10^{30}$ $\left[\text{g}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau\cdot 2^{3}5^{3}$ | Gauss |
| $1.898124(42) \times 10^{30}$ $\left[\text{g}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau\cdot 2^{3}5^{3}$ | LorentzHeaviside |
| $4.184647(92) \times 10^{27}$ $\left[\text{lb}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{lb}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | FPS |
| $1.083857(24) \times 10^{25}$ $\left[\text{slinch}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{g}_0^{-1}\text{ft}\cdot \text{lb}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau\cdot 2^{-2}3^{-1}$ | IPS |
| $1.300628(29) \times 10^{26}$ $\left[\text{slug}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{g}_0^{-1}\text{ft}\cdot \text{lb}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | British |
| $4.184647(92) \times 10^{27}$ $\left[\text{lbm}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{lb}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | English |
| $4.184647(92) \times 10^{27}$ $\left[\text{lbm}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{lb}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | Survey |
| $4.184647(92) \times 10^{27}$ $\left[\text{lb}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{lb}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | MPH |
| $1.898124(42) \times 10^{27}$ $\left[\text{kg}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau$ | KKH |
| $1.889902(42) \times 10^{27}$ $\left[\text{keg}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{g}_0^{3/2}\text{m}_\text{P}^{2}\text{GM}_\text{E}^{-3/2}\text{GM}_\text{J}\cdot \tau^{-2}2^{27}5^{21}$ | Nautical |
| $1.889902(42) \times 10^{27}$ $\left[\text{keg}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{g}_0^{3/2}\text{m}_\text{P}^{2}\text{GM}_\text{E}^{-3/2}\text{GM}_\text{J}\cdot \tau^{-2}2^{27}5^{21}$ | Meridian |
| $0.000954594262(68)$ $\left[\text{M}_\odot\right]$ | $\text{au}^{-3}\text{k}_\text{G}^{-2}\text{GM}_\text{J}\cdot \tau^{-2}2^{28}3^{14}5^{10}$ | IAU☉ |
| $317.828383(23)$ $\left[\text{ME}\right]$ | $\text{GM}_\text{E}^{-1}\text{GM}_\text{J}$ | IAUE |
| $1.0$ $\left[\text{MJ}\right]$ | $1$ | IAUJ |
| $2.083702(46) \times 10^{57}$ $\left[\mathbb{1}\right]$ | $\hbar^{-2}\text{R}_{\infty}^{-1}\alpha^{2}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau\cdot 2^{-1}$ | Hubble |
| $7.430(55) \times 10^{-26}$ $\left[\text{M}\right]$ | $\text{c}^{-3}\Omega_{\Lambda}^{1/2}\text{H}_0\cdot \text{au}^{-1}\text{GM}_\text{J}\cdot \tau^{3/2}2^{-9}3^{-7/2}5^{-6}$ | Cosmological |
| $4.737(18) \times 10^{65}$ $\left[\text{M}\right]$ | $\hbar^{-3/2}\Omega_{\Lambda}^{-1/4}\text{H}_0^{-1/2}\text{au}^{1/2}\text{m}_\text{P}^{3/2}\text{GM}_\text{J}\cdot \tau^{5/4}2^{11/2}3^{7/4}5^{3}$ | CosmologicalQuantum |
| $3.091605(34) \times 10^{35}$ $\left[\text{M}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}\cdot \text{GM}_\text{J}\cdot \tau^{3/2}2^{1/2}$ | Planck |
| $8.721257(96) \times 10^{34}$ $\left[\text{m}_\text{P}\right]$ | $\hbar^{-1}\text{c}^{-1}\text{m}_\text{P}\cdot \text{GM}_\text{J}\cdot \tau$ | PlanckGauss |
| $1.020931(11) \times 10^{36}$ $\left[\text{M}\right]$ | $\hbar^{-1}\text{c}^{-1}\alpha^{-1/2}\text{m}_\text{P}\cdot \text{GM}_\text{J}\cdot \tau$ | Stoney |
| $2.083702(46) \times 10^{57}$ $\left[\mathbb{1}\right]$ | $\hbar^{-2}\text{R}_{\infty}^{-1}\alpha^{2}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau\cdot 2^{-1}$ | Hartree |
| $1.041851(23) \times 10^{57}$ $\left[\text{M}\right]$ | $\hbar^{-2}\text{R}_{\infty}^{-1}\alpha^{2}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau\cdot 2^{-2}$ | Rydberg |
| $1.020931(11) \times 10^{36}$ $\left[\text{M}\right]$ | $\hbar^{-1}\text{c}^{-1}\alpha^{-1/2}\text{m}_\text{P}\cdot \text{GM}_\text{J}\cdot \tau$ | Schrodinger |
| $2.083702(46) \times 10^{57}$ $\left[\mathbb{1}\right]$ | $\hbar^{-2}\text{R}_{\infty}^{-1}\alpha^{2}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau\cdot 2^{-1}$ | Electronic |
| $2.083702(46) \times 10^{57}$ $\left[\mathbb{1}\right]$ | $\hbar^{-2}\text{R}_{\infty}^{-1}\alpha^{2}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau\cdot 2^{-1}$ | Natural |
| $2.083702(46) \times 10^{57}$ $\left[\mathbb{1}\right]$ | $\hbar^{-2}\text{R}_{\infty}^{-1}\alpha^{2}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau\cdot 2^{-1}$ | NaturalGauss |
| $1.134820(25) \times 10^{54}$ $\left[\text{m}_\text{p}\right]$ | $\hbar^{-2}\text{R}_{\infty}^{-1}\alpha^{2}\mu_\text{eu}\cdot \mu_\text{pu}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau\cdot 2^{-1}$ | QCD |
| $1.134820(25) \times 10^{54}$ $\left[\text{m}_\text{p}\right]$ | $\hbar^{-2}\text{R}_{\infty}^{-1}\alpha^{2}\mu_\text{eu}\cdot \mu_\text{pu}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau\cdot 2^{-1}$ | QCDGauss |
| $1.134820(25) \times 10^{54}$ $\left[\text{m}_\text{p}\right]$ | $\hbar^{-2}\text{R}_{\infty}^{-1}\alpha^{2}\mu_\text{eu}\cdot \mu_\text{pu}^{-1}\text{m}_\text{P}^{2}\text{GM}_\text{J}\cdot \tau\cdot 2^{-1}$ | QCDoriginal |