Schwarzschild Radius of the Sun
| Value | 2953.25 m |
| Status | Measured: ± 0.01 m (0.0000034 relative) |
| Source | Derived from JPL DE440 GM⊙ and the defined speed of light |
| Categories | Astronomicalrelativitystellar |
| femtometer | 2.9532500e+18 fm |
| picometer | 2.9532500e+15 pm |
| nanometer | 2,953,250,000,000 nm |
| micrometer | 2,953,250,000 μm |
| millimeter | 2,953,250 mm |
| centimeter | 295,325 cm |
| decimeter | 29,532.5 dm |
| meter | 2,953.25 m |
| kilometer | 2.95325 km |
| inch | 116,269.69 in |
| foot | 9,689.1404 ft |
| yard | 3,229.7135 yd |
| mile | 1.8350645 mi |
| nautical mile | 1.5946274 nmi |
| astronomical unit | 1.9741257e-08 AU |
| light-year | 3.1215877e-13 ly |
| parsec | 9.5708314e-14 pc |
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.