True Field of View Calculator

Calculate how much actual sky an eyepiece shows — true field ≈ apparent field ÷ magnification, or the more accurate 57.2958 × field stop ÷ telescope focal length when the field stop is known — in degrees and arcminutes, with the Moon, Andromeda Galaxy, Orion Nebula, Pleiades, and the Double Cluster drawn to scale inside the resulting field to answer 'will it fit' directly.

True field of view calculator

TFOV ≈ AFOV / M from the eyepiece's apparent field, or the more accurate TFOV = 57.2958 × field stop / F when the eyepiece's physical field stop is known. The number matters less than the picture: how much sky actually fits.

mm
mm
°
mm
TFOV ≈ 1.289° (77.3′)
at 50× magnification
Simple (AFOV/M): 1.36°Field-stop: 1.289°5.495% apart
eyepiece field — 1.289°
  • average apparent diameterFits
  • full naked-eye cluster extent (≈110′)Too wide
  • bright nebulosity extent (≈65′×60′)Fits
  • full cataloged extent (≈190′×60′) — the bright core alone looks much smallerToo wide
  • each cluster ≈30′ across, centers ≈30′ apartFits

Every shape is drawn to the same angular scale as the field-of-view circle — an object that pokes outside it genuinely doesn't fit in one view, no diagram trick.

Magnification gets all the attention, but it isn’t the number that decides whether the Pleiades fit in one view or whether you’ll be panning the telescope across Andromeda in three separate passes. That’s true field of view — how much actual sky is visible through the eyepiece — and it shrinks as magnification grows, not the other way around most people assume.

The simple method

TFOVAFOVM\text{TFOV} \approx \frac{\text{AFOV}}{M}

AFOV is the eyepiece’s own apparent field of view — how wide the view feels looking through it, printed on nearly every eyepiece’s spec sheet — and M is the magnification (telescope focal length over eyepiece focal length). A 25mm eyepiece with a 52° apparent field, used at 40×, shows 52/40 ≈ 1.3° of actual sky.

The more accurate method

TFOV=57.2958×field stop (mm)F (mm)\text{TFOV} = 57.2958 \times \frac{\text{field stop (mm)}}{F\ (\text{mm})}

The field stop is a physical aperture inside the eyepiece barrel that defines the sharp edge of the view — a real, measurable diameter in millimeters, not a spec-sheet number. 57.2958 is 180/π, converting the small-angle relation (field stop divided by the telescope’s focal length, in radians) to degrees. A manufacturer’s stated AFOV is sometimes rounded, and for wide-angle designs with real optical distortion at the edge of the field it can diverge from the field-stop figure by several percent — the Tele Vue Panoptic 24mm preset here is a real eyepiece where that gap is close to 5%. When both numbers are available, the field-stop method is the one to trust.

Both methods are Kepler’s third law’s small-angle cousin applied to eyepiece optics rather than orbits — for the underlying angular-size relation itself, exact rather than approximated, see this site’s Angular Size & Physical Size Calculator, which supplies the same real angular diameters used in the overlay below. And because true field falls as magnification rises, it’s worth reading together with the Telescope Magnification & Eyepiece Calculator: the same eyepiece swap that pushes you toward empty magnification is also shrinking your field down to a fraction of what it was.

Reading the overlay

The real payoff isn’t the degree number, it’s the picture: the dashed circle is the eyepiece’s field of view, and each shaded shape is a well-known object’s real apparent size, drawn to that exact same angular scale and centered together. An object whose outline pokes past the dashed circle genuinely doesn’t fit in one view — no illustration trick, just the same angle measured two ways. Toggle any of the Moon, the Pleiades, the Orion Nebula, the Andromeda Galaxy, or the Double Cluster on or off from the legend to compare them directly against your own setup, or against each other.

Two things worth noticing: Andromeda’s full cataloged extent (about 3° across) doesn’t fit inside most eyepieces’ fields at any reasonable magnification — only its brighter core, much smaller, is what most observers actually see and recognize. And at high enough power, the Moon itself stops fitting — the “10mm planetary eyepiece” preset here frames a field narrower than the Moon’s own apparent diameter, which is exactly why lunar observers back off to lower power to see the whole disk at once.

View source on GitHub

Changelog

  • 2026-08-31Published.