Einstein Ring Angular Radius Calculator

Calculate the Einstein ring radius for gravitational lensing.
Enter lens mass and distances to find the angular radius in arcseconds.

Nearby, this is simply D_S minus D_L. At cosmological distances angular-diameter distances do not add, so look it up rather than subtracting.
Einstein Ring Radius

Gravitational lensing occurs when a massive object bends the light from a more distant source. When the source, lens, and observer are perfectly aligned, the source appears as a ring, an Einstein ring.

Einstein ring angular radius:

θ_E = √(4GM/c² × D_LS / (D_L × D_S))

In arcseconds, with all three distances in kiloparsecs and the mass in solar masses:

θ_E ≈ 0.002854" × √(M/M☉ × D_LS / (D_L × D_S))

Sanity check that coefficient against a realistic case: a 10¹¹ M☉ galaxy a gigaparsec away (D_L = 10⁶ kpc) lensing a source at D_S = 2 × 10⁶ kpc, with D_LS = 10⁶ kpc, gives 0.002854 × √(10¹¹ × 5 × 10⁻⁷) = 0.002854 × 223.6 = 0.64 arcseconds. That is the scale real galaxy-galaxy lenses are found at, and it is why they need Hubble or adaptive optics to resolve. If you see this written with a coefficient near 0.9, that version is for mass in units of 10¹¹ M☉ and distances in gigaparsecs. Mixing the two up moves the answer by a factor of about 300.

Put the same galaxy a thousand times closer, at 1000 kpc, and the ring swells to 20 arcseconds. Nothing is wrong with the arithmetic; it is just that no galaxy that near is lined up behind anything, so rings that large in practice come from clusters rather than single galaxies.

Where:

  • D_L = distance from observer to lens (lensing object)
  • D_S = distance from observer to source
  • D_LS = distance from lens to source

What it tells us: The Einstein radius defines the region of maximum magnification. Light sources within θ_E of the lens-observer line are strongly magnified. Objects further than θ_E are weakly lensed.

Physical Einstein radius: The actual physical size of the Einstein ring on the lens plane:

R_E = θ_E × D_L (in AU or km)

Famous Einstein rings:

  • B1938+666: one of the first complete Einstein rings discovered (1998)
  • SDSS J0946+1006: a “double Einstein ring” with two lensed galaxies
  • Gravitational lensing has been observed for everything from stars (microlensing) to entire galaxy clusters

Microlensing: When a compact object (star, brown dwarf, or planet) passes in front of a background star, the Einstein radius determines the magnification event duration. Used to detect dark matter candidates and extrasolar planets.


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This calculator runs entirely in your browser, so the numbers you enter stay on your device. The math behind it is written by hand and tested against worked examples and standard references before the page goes live.

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