Schwarzschild Radius of the Sun

rs,=2953.25 mr_{s,\odot} = 2953.25\ \text{m}
Value2953.25 m
StatusMeasured: ± 0.01 m (0.0000034 relative)
SourceDerived from JPL DE440 GM⊙ and the defined speed of light
CategoriesAstronomicalrelativitystellar
r_s_sun in every length unit
femtometer2.9532500e+18 fm
picometer2.9532500e+15 pm
nanometer2,953,250,000,000 nm
micrometer2,953,250,000 μm
millimeter2,953,250 mm
centimeter295,325 cm
decimeter29,532.5 dm
meter2,953.25 m
kilometer2.95325 km
inch116,269.69 in
foot9,689.1404 ft
yard3,229.7135 yd
mile1.8350645 mi
nautical mile1.5946274 nmi
astronomical unit1.9741257e-08 AU
light-year3.1215877e-13 ly
parsec9.5708314e-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.