great circle unit
data derived with UnitSystems.jl
\[\text{L}\]
\[\left[\hbar\cdot \text{c}^{-1}\text{m}_\text{e}^{-1}\phi\cdot \text{g}_0\right]\]
| Quantity | Product | UnitSystem |
|---|---|---|
| $4.0057922172(40) \times 10^{7}$ $\left[\text{m}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau$ | Metric |
| $4.0057922172(40) \times 10^{7}$ $\left[\text{m}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau$ | SI2019 |
| $4.0057922172(40) \times 10^{7}$ $\left[\text{m}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau$ | SI1976 |
| $4.0057922172(40) \times 10^{7}$ $\left[\text{m}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau$ | CODATA |
| $4.0057922172(40) \times 10^{7}$ $\left[\text{m}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau$ | Conventional |
| $4.0057922172(40) \times 10^{7}$ $\left[\text{m}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau$ | International |
| $4.0057922172(40) \times 10^{7}$ $\left[\text{m}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau$ | InternationalMean |
| $4.0057922172(40) \times 10^{7}$ $\left[\text{m}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau$ | MetricTurn |
| $4.0057922172(40) \times 10^{7}$ $\left[\text{m}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau$ | MetricSpatian |
| $4.0057922172(40) \times 10^{7}$ $\left[\text{m}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau$ | MetricGradian |
| $4.0057922172(40) \times 10^{7}$ $\left[\text{m}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau$ | MetricDegree |
| $4.0057922172(40) \times 10^{7}$ $\left[\text{m}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau$ | MetricArcminute |
| $4.0057922172(40) \times 10^{7}$ $\left[\text{m}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau$ | MetricArcsecond |
| $4.0057922172(40) \times 10^{7}$ $\left[\text{m}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau$ | Engineering |
| $4.0057922172(40) \times 10^{7}$ $\left[\text{m}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau$ | Gravitational |
| $4.0057922172(40) \times 10^{7}$ $\left[\text{m}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau$ | MTS |
| $4.0057922172(40) \times 10^{9}$ $\left[\text{cm}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau\cdot 2^{2}5^{2}$ | EMU |
| $4.0057922172(40) \times 10^{9}$ $\left[\text{cm}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau\cdot 2^{2}5^{2}$ | ESU |
| $4.0057922172(40) \times 10^{9}$ $\left[\text{cm}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau\cdot 2^{2}5^{2}$ | Gauss |
| $4.0057922172(40) \times 10^{9}$ $\left[\text{cm}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau\cdot 2^{2}5^{2}$ | LorentzHeaviside |
| $1.3142362917(13) \times 10^{8}$ $\left[\text{ft}\right]$ | $\text{g}_0^{-1/2}\text{ft}^{-1}\text{GM}_\text{E}^{1/2}\tau$ | FPS |
| $1.5770835501(16) \times 10^{9}$ $\left[\text{in}\right]$ | $\text{g}_0^{-1/2}\text{ft}^{-1}\text{GM}_\text{E}^{1/2}\tau\cdot 2^{2}3$ | IPS |
| $1.3142362917(13) \times 10^{8}$ $\left[\text{ft}\right]$ | $\text{g}_0^{-1/2}\text{ft}^{-1}\text{GM}_\text{E}^{1/2}\tau$ | British |
| $1.3142362917(13) \times 10^{8}$ $\left[\text{ft}\right]$ | $\text{g}_0^{-1/2}\text{ft}^{-1}\text{GM}_\text{E}^{1/2}\tau$ | English |
| $1.3142336633(13) \times 10^{8}$ $\left[\text{ft}\right]$ | $\text{g}_0^{-1/2}\text{ft}_\text{US}^{-1}\text{GM}_\text{E}^{1/2}\tau$ | Survey |
| $24890.8388590(25)$ $\left[\text{mi}\right]$ | $\text{g}_0^{-1/2}\text{ft}^{-1}\text{GM}_\text{E}^{1/2}\tau\cdot 2^{-5}3^{-1}5^{-1}11^{-1}$ | MPH |
| $40057.922172(40)$ $\left[\text{km}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau\cdot 2^{-3}5^{-3}$ | KKH |
| $21600.0$ $\left[\text{nm}\right]$ | $2^{5}3^{3}5^{2}$ | Nautical |
| $4.0 \times 10^{7}$ $\left[\text{em}\right]$ | $2^{9}5^{7}$ | Meridian |
| $0.00026777067070(27)$ $\left[\text{au}\right]$ | $\text{g}_0^{-1/2}\text{au}^{-1}\text{GM}_\text{E}^{1/2}\tau$ | IAU☉ |
| $0.10420922576(10)$ $\left[\text{LD}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau\cdot 2^{-3}3^{-3}5^{-3}/14237$ | IAUE |
| $5.1456650946(52) \times 10^{-5}$ $\left[\text{JD}\right]$ | $\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau\cdot 2^{-6}3^{-1}5^{-6}/259493$ | IAUJ |
| $2.930(18) \times 10^{-19}$ $\left[\text{T}\right]$ | $\text{c}^{-1}\text{H}_0\cdot \text{g}_0^{-1/2}\text{au}^{-1}\text{GM}_\text{E}^{1/2}\tau^{2}2^{-10}3^{-4}5^{-6}$ | Hubble |
| $8.402(62) \times 10^{-20}$ $\left[\text{T}\right]$ | $\text{c}^{-1}\Omega_{\Lambda}^{1/2}\text{H}_0\cdot \text{g}_0^{-1/2}\text{au}^{-1}\text{GM}_\text{E}^{1/2}\tau^{3/2}2^{-11}3^{-7/2}5^{-6}$ | Cosmological |
| $4.563(17) \times 10^{11}$ $\left[\text{M}^{-1}\right]$ | $\hbar^{-1/2}\Omega_{\Lambda}^{1/4}\text{H}_0^{1/2}\text{g}_0^{-1/2}\text{au}^{-1/2}\text{m}_\text{P}^{1/2}\text{GM}_\text{E}^{1/2}\tau^{7/4}2^{-11/2}3^{-7/4}5^{-3}$ | CosmologicalQuantum |
| $6.991551(77) \times 10^{41}$ $\left[\text{M}^{-1}\right]$ | $\hbar^{-1}\text{c}\cdot \text{g}_0^{-1/2}\text{m}_\text{P}\cdot \text{GM}_\text{E}^{1/2}\tau^{3/2}2^{-1/2}$ | Planck |
| $2.478440(27) \times 10^{42}$ $\left[\text{m}_\text{P}^{-1}\right]$ | $\hbar^{-1}\text{c}\cdot \text{g}_0^{-1/2}\text{m}_\text{P}\cdot \text{GM}_\text{E}^{1/2}\tau^{2}$ | PlanckGauss |
| $2.901321(32) \times 10^{43}$ $\left[\text{T}\right]$ | $\hbar^{-1}\text{c}\cdot \alpha^{-1/2}\text{g}_0^{-1/2}\text{m}_\text{P}\cdot \text{GM}_\text{E}^{1/2}\tau^{2}$ | Stoney |
| $7.5698502027(77) \times 10^{17}$ $\left[\text{a}_0\right]$ | $\text{R}_{\infty}\cdot \alpha^{-1}\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau^{2}2$ | Hartree |
| $7.5698502027(77) \times 10^{17}$ $\left[\text{a}_0\right]$ | $\text{R}_{\infty}\cdot \alpha^{-1}\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau^{2}2$ | Rydberg |
| $1.544993(17) \times 10^{39}$ $\left[\text{L}\right]$ | $\hbar^{-1}\text{c}\cdot \alpha^{3/2}\text{g}_0^{-1/2}\text{m}_\text{P}\cdot \text{GM}_\text{E}^{1/2}\tau^{2}$ | Schrodinger |
| $1.4215319537(16) \times 10^{22}$ $\left[\text{T}\right]$ | $\text{R}_{\infty}\cdot \alpha^{-3}\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau^{2}2$ | Electronic |
| $1.0373419854(11) \times 10^{20}$ $\left[\mathbb{1}\right]$ | $\text{R}_{\infty}\cdot \alpha^{-2}\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau^{2}2$ | Natural |
| $1.0373419854(11) \times 10^{20}$ $\left[\mathbb{1}\right]$ | $\text{R}_{\infty}\cdot \alpha^{-2}\text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau^{2}2$ | NaturalGauss |
| $1.9047182598(20) \times 10^{23}$ $\left[\text{m}_\text{p}^{-1}\right]$ | $\text{R}_{\infty}\cdot \alpha^{-2}\mu_\text{eu}^{-1}\mu_\text{pu}\cdot \text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau^{2}2$ | QCD |
| $1.9047182598(20) \times 10^{23}$ $\left[\text{m}_\text{p}^{-1}\right]$ | $\text{R}_{\infty}\cdot \alpha^{-2}\mu_\text{eu}^{-1}\mu_\text{pu}\cdot \text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau^{2}2$ | QCDGauss |
| $1.9047182598(20) \times 10^{23}$ $\left[\text{m}_\text{p}^{-1}\right]$ | $\text{R}_{\infty}\cdot \alpha^{-2}\mu_\text{eu}^{-1}\mu_\text{pu}\cdot \text{g}_0^{-1/2}\text{GM}_\text{E}^{1/2}\tau^{2}2$ | QCDoriginal |