Observational Bulletin / No. 618
Cosmic Hypothetical
Hypercompact Quasar / 4 × 10¹⁰ M☉

A question of distance.

TON 618 sits 10.4 billion light-years away and still registers in modest telescopes. Bring it closer and the calculus inverts: at some point the view is sublime, then it cooks the planet, then it eats us. Move the dial.

Field of view: 4°
Moon · 0.5° · for scale
TON 618

Distance

Drag the slider · Tap a landmark
Distance from Earth 3,000 ly
Apparent Magnitude
−16.8
brighter than the full moon
Angular Diameter
6.9
resolvable in binoculars
Brightness vs. Moon
63×
casts hard shadows
Habitability
Tense
solar system intact
Verdict Spectacular

A glowing disk pinned to the night sky, brighter than the moon, faintly resolved as a structure rather than a point. The accretion ring is visible. Two pencil-thin jets extend perpendicular for arc-minutes. Earth is fine. The Oort cloud is being slowly stripped, but on geological timescales.

Working it out.

Live values at 3,000 ly
01 / Brightness
Apparent magnitude
m  =  m0  +  5 log10 (d / d0)

A logarithmic scale where every 5 magnitudes is a factor of 100 in brightness, and lower numbers are brighter. The Sun is −26.7, the full moon −12.7, the faintest naked-eye star +6. Starting from TON 618's measured magnitude at its real distance, we just rescale by inverse-square dimming.

Worked out
m = 15.9 + 5·log10(3,000 / 1.04×10¹⁰) = 15.9 + 5·(−6.54) = 15.9 + (−32.69) = −16.79
02 / Apparent size
Angular diameter
θ  =  (D / d) × 206,265 ″

The disk's physical diameter divided by its distance gives an angle in radians. The constant 206,265 just converts radians to arcseconds, the unit astronomers use for tiny angles. The full moon spans about 1,800″ (half a degree). Naked-eye resolution maxes out around 60″.

Worked out
θ = (0.1 ly / 3,000 ly) × 206,265 = 3.33×10⁻⁵ × 206,265 = 6.88″
03 / Comparison
Brightness vs. the Moon
R  =  10(mmoonmTON) / 2.5

The Pogson relation, which inverts the magnitude scale into a flux ratio. A 5-magnitude difference is exactly 100×. Negative ratios don't exist; the formula is built so that brighter wins, regardless of which side has the lower number.

Worked out
R = 10^((−12.7 − (−16.79)) / 2.5) = 10^(4.09 / 2.5) = 10^1.64 = ≈ 43×
04 / Gravity
The Sun's Hill sphere
rH  =  a · (m / 3M)1/3

The radius around the Sun where its gravity still wins against TON 618's. Beyond this, an object is no longer bound to us. The cube-root scaling makes this the most forgiving of the gravitational effects, but it shrinks fast as TON 618 gets closer. Today's value (against the galactic potential) is roughly 4 ly.

Worked out
rH = 3,000 ly × (1 / (3·4×10¹⁰))1/3 = 1.90×10⁸ AU × 2.03×10⁻⁴ = ≈ 38,500 AU Oort cloud reaches ~100,000 AU. Kuiper belt ends near 1,000 AU.

For context.

An aside / Why we're here
A / What it is

A black hole, a disk, and a lot of light

TON 618 is a quasar, an active galactic nucleus powered by one of the most massive black holes ever measured at roughly 40 billion solar masses. The "TON" comes from the Tonantzintla catalogue, compiled at a Mexican observatory in the late 1950s, where it was first noted as a faint blue object. Decades later, spectroscopy revealed the absurdity of the thing. Its accretion disk outshines the entire Milky Way by a factor of about 140 trillion to one.

B / How far

Near the edge of what we can see

Roughly 10.4 billion light-years away, with a redshift of z = 2.219. The photons reaching telescopes today left TON 618 when the universe was less than a third of its current age. Because space has been expanding the whole time, its present location has drifted to about 18 billion light-years from us. It is one of the most distant individual objects easily picked up by amateur astronomy.

C / Where this came from

A tweet, basically

The premise of this page was a tweet that pointed out: if TON 618 sat where Alpha Centauri does (4.37 ly), the night sky would be unrecognizable. That is correct, and a wild understatement. The conversation that followed worked through gravity, then radiation, then the math. This page is the visual version. Move the slider. Watch the universe break.

✦ · ✦ · ✦

From Sol to TON 618

A chart of the void · waypoints not to scale

The receipts.

References & assumptions

Numbers used

Black hole mass: ~40 billion M☉
Estimates range from 40 to 66 billion solar masses. Lower figure: Xue Ge et al. (2019) using C IV emission lines. Higher: Shemmer et al. (2004) via Hβ. The math here uses 40B; recompute with 66B and the Hill sphere shrinks by ~16%.
en.wikipedia.org/wiki/TON_618
Distance: 10.4 Gly light-travel
Redshift z = 2.219. Light-travel time ~10.8 Gyr; comoving distance ~18.2 Gly. Standard ΛCDM cosmology (H₀ ≈ 70 km/s/Mpc).
en.wikipedia.org/wiki/TON_618
Bolometric luminosity: 4 × 10⁴⁰ W
Roughly 140 trillion solar luminosities. Absolute magnitude −30.7. Apparent magnitude V = 15.9.
en.wikipedia.org/wiki/TON_618
Discovery: 1957 / 1970
First catalogued 1957 (Tonantzintla Observatory, Mexico) by Iriarte and Chavira as a faint blue object. Identified as a quasar in 1970 after radio detection.
skyatnightmagazine.com/space-science/ton-618
Standard formulas: textbook physics
Distance modulus, Pogson relation (1856), angular diameter, and Hill sphere are all classical astrodynamics. Any introductory astrophysics text. Inverse-square dimming assumes negligible interstellar extinction at these scales.

Honest caveats

On the disk size.
The 0.1 ly figure is an order-of-magnitude approximation for the visible accretion structure. The Schwarzschild radius alone is 0.02 ly (1,300 AU), and the broad-line region extends well beyond that. The disk's true diameter is poorly constrained by direct observation. If you object, halve or double it; the angular sizes scale linearly.
On the habitability thresholds.
The "Lethal", "Tense", "Vivid" verdicts are gut-feel translations of radiation flux and gravitational influence, not rigorous astrobiology. The orders of magnitude are right; the exact distance boundaries are interpretive.
On the Hill sphere math.
Treats both Sol and TON 618 as point masses with TON 618 stationary, which is the standard idealization. Real perturbations would also depend on relative motion, the galactic potential, and the structure of TON 618's host galaxy. Useful for intuition, not for plotting cometary trajectories.
For the curious, not the rigorous.
This page is editorial science writing. Where the literature disagreed, the friendlier or more familiar number was preferred. Where assumptions were necessary, they're stated. Corrections welcome; pretensions to peer review, not.