Schwarzschild Radius of the Sun
| Value | 2,953.25 m |
| Status | Measured: ± 0.01 m (0.0000034 relative) |
| Source | Derived from JPL DE440 GM⊙ and the defined speed of light |
| Categories | AstronomicalStars & Sun |
| Planck length | 1.8272179e+38 lP |
| femtometer | 2.9532500e+18 fm |
| picometer | 2.9532500e+15 pm |
| bohr radius | 55,808,337,000,000 a0 |
| angstrom | 29,532,500,000,000 Å |
| nanometer | 2,953,250,000,000 nm |
| micrometer | 2,953,250,000 μm |
| thou | 116,269,690 thou |
| point | 8,371,417.3 pt |
| millimeter | 2,953,250 mm |
| pica | 697,618.11 pc |
| centimeter | 295,325 cm |
| inch | 116,269.69 in |
| decimeter | 29,532.5 dm |
| hand | 29,067.421 hh |
| link | 14,680.516 li |
| foot | 9,689.1404 ft |
| US survey foot | 9,689.121 ftUS |
| yard | 3,229.7135 yd |
| meter | 2,953.25 m |
| fathom | 1,614.8567 ftm |
| rod | 587.22063 rd |
| chain | 146.80516 ch |
| cable length | 15.946274 cb |
| furlong | 14.680516 fur |
| kilometer | 2.95325 km |
| mile | 1.8350645 mi |
| nautical mile | 1.5946274 nmi |
| league | 0.61168816 lea |
| megameter | 0.00295325 Mm |
| Earth radius | 0.00046354575 REarth |
| light-second | 0.0000098509816 ls |
| lunar distance | 0.0000076827723 LD |
| solar radius | 0.000004245005 Rsun |
| light-minute | 1.6418303e-07 lmin |
| astronomical unit | 1.9741257e-08 AU |
| light-year | 3.1215877e-13 ly |
| parsec | 9.5708314e-14 pc |
| kiloparsec | 9.5708314e-17 kpc |
| megaparsec | 9.5708314e-20 Mpc |
| gigaparsec | 9.5708314e-23 Gpc |
Learning zone
Karl Schwarzschild solved Einstein's field equations in 1915 within weeks of their publication, while serving on the Russian front, and found that a mass squeezed inside r = 2GM/c² curves spacetime so severely that no signal can climb back out. Put the Sun's mass parameter in and the answer is 2.95 km — the Sun would have to shrink by a factor of 235 000 to reach it, which it never will; a star of one solar mass ends as a white dwarf about the size of Earth.
The radius scales linearly with mass, which makes the ratio r_s/r a handy measure of how relativistic a system is. At the Sun's actual surface that ratio is 4 × 10⁻⁶, and it is exactly what produces the 1.75-arcsecond deflection of starlight that Eddington's 1919 eclipse expedition measured, and the 43 arcseconds per century of Mercury's perihelion advance that Newton could not explain.