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C-mount camera on a telescope: adapters and back focus

The C-mount camera to 1.25-inch telescope adapter choice, the 17.526 mm back-focus math, vignetting by sensor size, and a sampling example with the arithmetic.

LumaSpec Vision11 min read Share on LinkedIn

On this page 9 sections
  1. 01Which adapter puts a C-mount camera on a telescope?
  2. 02How does back focus work with no lens in the path?
  3. 03Will a 1.25-inch focuser vignette the sensor?
  4. 04What field of view and sampling does prime focus give?
    1. Worked example: a 200 mm aperture at f/10 and at f/5
  5. 05When is eyepiece projection better than prime focus?
  6. 06Which camera suits a telescope?
  7. 07How do you reach focus and check the image?
  8. 08What do you check before ordering?
  9. 09Questions

A C-mount machine-vision camera bolts straight onto a telescope: the scope is just a very long focal length with no mount of its own, and one small adapter bridges the two worlds. This guide is for anyone pointing a GigE or USB3 area-scan camera at the Moon, at the Sun behind a proper front filter, or at a deep-sky target. You will pick the right adapter, land the sensor exactly on the focal plane, keep a 1.25-inch barrel from clipping the corners, and compute the sampling you actually get, with the arithmetic shown.

Which adapter puts a C-mount camera on a telescope?

A C-mount-to-1.25-inch prime-focus adapter is the standard coupling. Its 31.75 mm nose barrel slides into the focuser where an eyepiece would sit, and its female C-mount thread, one inch with 32 threads per inch, takes the camera body directly.

Prime focus means no glass in the adapter: the telescope objective forms the image on the sensor by itself, in the role a machine-vision lens plays on the bench. Three nose sizes cover almost every focuser: 24.5 mm (0.965 inch), 31.75 mm (1.25 inch) and 50.8 mm (2 inch), with 1.25 inch the common default. Many adapters carry a T2 female thread, M42 × 0.75, on the camera side instead, and a T2-to-C-mount ring completes that path. Optically the two routes are identical, so nose size and thread are the only decisions.

Check the camera side first. A true C-mount camera sits its sensor 17.526 mm behind the mounting face, a CS-mount body 5 mm closer, so a CS camera on a C-thread adapter needs a 5 mm spacer ring — the full comparison is in C mount vs CS mount: adapters, focus and clearance. The camera side of the joint is our territory: the lens accessories range holds the rings, tubes and filters, while the nosepiece adapter itself comes from telescope dealers, so measure the focuser before you order.

How does back focus work with no lens in the path?

With nothing between objective and sensor, the sensor must land exactly on the telescope focal plane. The camera holds it 17.526 mm behind the C-mount face, the adapter adds its own fixed optical path, and the focuser drawtube carries the last millimeters.

A typical adapter path runs 20-35 mm, so the whole stack reaches about 40-50 mm in front of the sensor; that total is the number to compare against your scope's usable back focus. Catadioptric tubes — Schmidt-Cassegrains and Maksutovs — focus by moving the primary mirror, so they travel generously in both directions and forgive tall stacks. Refractors and Newtonians hold a fixed focal plane and offer only the drawtube travel, a few tens of millimeters on most focusers.

Two failure directions, two fixes. If the focal plane sits farther out than the fully racked-out drawtube reaches, add spacing behind the camera: a 15 mm C-mount extension tube (LS-LXR-0255) moves the sensor 15 mm outward and hands back the missing travel, the same arithmetic as in lens extension tubes for close-up machine vision. If the stack is too tall and the sensor cannot rack in low enough — the classic Newtonian complaint — no spacer helps: buy the lowest-profile adapter available, and read the symptom the way you read a lens that only focuses at close distance, as a focus range that ends too early. The flange-distance bookkeeping is identical to checking adapter fit and flange distance on a camera body.

For the outward case, a printed-length spacer is the entire fix:

Lens accessoriesC-mount extension tubes, 15 mm (LS-LXR-0255)LS-LXR-0255
Type
Extension tubes
$79.00View partBuild a system with it

Will a 1.25-inch focuser vignette the sensor?

Yes for anything larger than a 2/3-inch sensor. A 1.25-inch barrel passes roughly a 25-30 mm clear cone, so an 11 mm diagonal fills it, a 1-inch sensor's 16 mm diagonal loses the corners, and the fix is a 2-inch (50.8 mm) focuser and adapter.

Sensor diagonals for the common formats: 1/2 inch is about 8 mm, 1/1.8 inch and 1/1.7 inch about 9 mm, 2/3 inch about 11 mm, 1 inch about 16 mm, 1.1 inch about 17.5 mm — the mapping from format name to glass size is in lens sensor format: 1/1.8, 2/3 and 1 inch lenses explained. Everything up to 2/3 inch passes a 1.25-inch barrel cleanly; 1 inch and larger want the 2-inch path. The drawtube inner shoulder is often the tighter stop, around 24-25 mm on older units, so hold a ruler across the focuser mouth before ordering anything above 2/3 inch. Gradual falloff divides out with flat frames; hard corner clipping does not, because those corners never received light.

What field of view and sampling does prime focus give?

The telescope replaces the lens. A 2000 mm focal length with a 2/3-inch sensor frames about 14.5 × 12.2 arcminutes, and 3.45 µm pixels at f/10 sample the diffraction spot 3.9 pixels across, which is oversampled by about 2×.

FOV [rad] ≈ sensor width [mm] / focal length [mm] image scale [arcsec/px] = 206.265 × pixel pitch [µm] / focal length [mm] Airy spot diameter [µm] = 2.44 × wavelength [µm] × f-number

Worked example: a 200 mm aperture at f/10 and at f/5

  • Focal length: 200 mm × 10 = 2000 mm.
  • Image scale: 206.265 × 3.45 / 2000 = 0.36 arcsec per pixel.
  • Airy spot at 550 nm: 2.44 × 0.55 × 10 = 13.4 µm, so 13.4 / 3.45 = 3.9 pixels per spot.
  • Bin 2 × 2 and the pixels act as 6.9 µm: scale 0.71 arcsec per pixel, spot 13.4 / 6.9 = 1.9 pixels, right at the Nyquist point.
  • At f/5 the same tube works at 1000 mm: scale 206.265 × 3.45 / 1000 = 0.71 arcsec per pixel, Airy spot 6.7 µm = 1.9 pixels. The 2/3-inch frame widens from 14.5 × 12.2 to 29 × 24 arcminutes, just under the Moon's 31-arcminute disc.

Nyquist sampling puts about two pixels across the spot, so 3.45 µm pixels match the optics near f/5 and oversample from roughly f/7 upward. Planetary imagers push harder on purpose, to a focal ratio near 5 × pixel pitch in µm — about f/17 for 3.45 µm — and shrink the frames in processing; that is a lucky-imaging choice, not a default. For deep-sky targets, typical 2-4 arcsec seeing caps useful sampling near 1 arcsec per pixel, and anything finer divides the same blurred image into more, noisier pixels. The field-of-view-first logic is the same one behind how to choose a machine vision lens focal length, and exposure follows the lower f-number, more light rule as always.

Lens focal length, field of view and working distance
Units
Solve for
Focal length
– mm
Field of view
– mm
Working distance
– mm
Magnification
– x
Angle of view
– °
Pixel on the part
– mm

Thin-lens model: m = sensor width / field of view, f = WD × m / (1 + m). Accurate to a few percent above about 150 mm; check the lens's minimum object distance.

Find lenses with this focal length Open the full calculator

When is eyepiece projection better than prime focus?

Eyepiece projection earns its extra glass on small bright targets. A 25 mm eyepiece projecting onto a sensor 100 mm behind it magnifies by M = 100 / 25 - 1 = 3, so a 2000 mm f/10 scope works at 6000 mm effective focal length and f/30.

Magnification follows M = d / f_eyepiece - 1, with d the eyepiece-to-sensor distance, and both effective focal length and focal ratio multiply by M. At M = 3 the numbers are: image scale 206.265 × 3.45 / 6000 = 0.12 arcsec per pixel, Airy spot 2.44 × 0.55 × 30 = 40 µm, and (30 / 10)² = 9× less light per pixel than at f/10. That is deliberate oversampling for planets, double stars and solar detail, scaled down in processing afterwards. The costs are real: the image dims as the f-ratio climbs, spacing now sets magnification and must stay fixed, and unsteady seeing punishes long effective focal lengths first. Deep-sky targets stay at prime focus, where the shorter focal ratio keeps exposures short.

Which camera suits a telescope?

Choose on sensor size against the focuser, shutter against motion, and interface against cable run. A 1/1.7-inch to 2/3-inch global-shutter color body covers Moon and planets through a 1.25-inch barrel, while a 1-inch mono body does deep sky but needs the 2-inch path.

MV-CU020-90GC is a 2.5 MP global-shutter color camera on a 1/1.7-inch format over GigE, and its GMAX4002 sensor is the small-frame pick for lunar and planetary video. LS-CMR-0053 moves to 12 MP mono on a 1/1.7-inch format, an IMX226 with a rolling shutter at 9 fps over GigE; on a tracked mount that shutter is no obstacle for still targets. MV-CS200-10UM pairs a 20 MP mono IMX183 with USB3 on a 1-inch format. That is the deep-sky body, and it wants a 2-inch light path.

Industrial bodies are uncooled, which costs little where it matters: lunar and planetary exposures run in the milliseconds, and short deep-sky subs calibrate clean with dark frames. For many-minute exposures an astro-cooled camera holds less noise, but dark-frame subtraction still takes an industrial sensor most of the way. Mono sensors also see infrared that mirror and achromats focus differently — the filter fixes are in color camera near infrared imaging: IR-cut filter options. All three bodies come from the area scan cameras range, and the camera finder filters it by mount, format and interface.

The table pulls the three together:

Specification MV-CU020-90GC LS-CMR-0053 MV-CS200-10UM
Sensor type CMOS, global shutter CMOS CMOS, rolling shutter
Sensor model GMAX4002 IMX 226 Sony® IMX183
Pixel size 4 μm × 4 μm 1.85 μm x 1.85 μm 2.4 μm × 2.4 μm
Sensor size 1/1.7" 1/1.7" 1"
Resolution 2048 × 1200 4000 px x 3000 px 5472 × 3648
Max. frame rate 49 fps @ 2048 × 1200 Bayer GB 8 9 fps 19.2 fps @ 5472 × 3648 Mono 8
Dynamic range 66.9 dB 60.0 dB 65.5 dB
SNR 40.8 dB >38.5 dB 41.5 dB
Gain 0 dB to 11.1 dB – 0 dB to 24 dB
Exposure time 4 μs to 10 sec – 44 μs to 0.83 sec
Exposure mode Off/Once/Continuous exposure mode – Off/Once/Continuous exposure mode, supports Global Reset and Rolling
Pixel format Bayer GB 8/10/10Packed/12/12Packed – Mono 8/10/10Packed/12/12Packed
Price $309.00 $560.00 $759.00

Values as printed in each product's data sheet; open a part for its drawing and full specifications.

How do you reach focus and check the image?

Coarse-focus in daylight on a distant rooftop, then fine-focus on the live image of a bright star or the lunar terminator until a star's half-width stops shrinking. Recheck once the tube reaches night temperature, because cooling shifts the focal plane.

  1. Thread the adapter onto the camera and seat the nose in the focuser hand-tight; if it binds or grinds, stop and diagnose — the usual causes are the ones in camera lens mount thread binding: safe checks before fitting.
  2. Coarse-focus on a distant daylight target at low gain and a short exposure.
  3. Centre a bright star or the Moon's terminator and fine-focus while watching a star-width or FWHM readout in the live view.
  4. Approach final focus from the same direction every time: SCT focusers rock the primary mirror, and single-direction finishing hides that backlash.
  5. Capture the corners and compare edge to centre brightness to confirm the barrel is not clipping, then take flat frames while the set-up still stands.

What do you check before ordering?

Six measurements decide the purchase: the focuser nose size, the adapter optical path, the sensor diagonal, the camera thread, the shutter type, and where the cable will run.

  • Nose size — measure the eyepiece barrel you are replacing: 31.75 mm is 1.25 inch, 50.8 mm is 2 inch, 24.5 mm is 0.965 inch.
  • Back focus — adapter path plus 17.526 mm must fit inside the scope's usable range; SCTs forgive, Newtonians rarely do.
  • Sensor diagonal — up to about 11 mm passes a 1.25-inch barrel; larger needs the 2-inch path.
  • Thread — C-mount camera on a C-thread adapter; a CS-mount body adds a 5 mm ring.
  • Shutter and interface — global shutter for fast targets, rolling shutter is fine tracked; GigE for the long cable run to the mount, USB3 at the desk.
  • Cabling — leave slack toward the mount and tie the cable to the tube, not to the focuser knob.

Step through the camera configurator to size the body against your focuser, pick spacing parts in the accessories finder, and if the two measurements do not line up on paper, contact us with the focuser and sensor dimensions before ordering hardware.

Questions

Can I leave a machine-vision lens mounted in front of the telescope?

No. The telescope objective already forms the image at its own focal plane, and prime focus means the sensor receives that image directly with nothing in between. A camera lens in front adds a second optical system, blocks most of the aperture and cannot reach a shared focus. Remove the lens and thread the adapter straight onto the C-mount; the telescope now acts as the lens.

What adapter fits a 0.965-inch focuser?

Only a few. The 0.965-inch standard is a 24.5 mm barrel found mostly on small beginner telescopes, and most C-mount adapters are made for 31.75 mm and 50.8 mm barrels. The practical routes are a hybrid 0.965-to-1.25-inch holder fitted in the focuser, or replacing the focuser itself. Measure the barrel diameter before ordering anything.

Do I need an IR-cut filter with a mono sensor?

Usually yes. Mono sensors respond well past 800 nm, and both mirrors and achromat objectives bring infrared to a different focus than visible light, so unfiltered stars bloat and color work turns soft. An IR-cut filter in the nosepiece path restores the visible focus. Narrowband imaging is the exception, where a band-pass filter takes its place.

Is a Barlow lens simpler than eyepiece projection?

Often, yes. A Barlow is a fixed negative amplifier, typically 2× to 3×, that multiplies the effective focal ratio the same way projection does but with no eyepiece to select and less sensitivity to spacing. You give up projection's wide magnification range. For planetary video at a steady 2× to 3× amplification, a Barlow in a 1.25-inch nosepiece is the simpler optical train.

How many frames per second do planetary captures need?

Aim for 60 to 300 frames per second in bursts of a few thousand frames, which is what lucky imaging needs to outrun atmospheric wobble. Shrink the ROI to the planet, raise the gain, and let the small frame run fast: a 640 × 480 ROI reads several times faster than a full 2/3-inch frame at the same interface.