Optics Basics for Choosing Your First Telescope: Aperture, Focal Length, and F-Ratio

Capítulo 2

Estimated reading time: 7 minutes

+ Exercise

1) Aperture: the one number that most strongly predicts what you’ll see

What aperture is

Aperture is the diameter of the telescope’s main light-collecting optic: the front lens on a refractor or the primary mirror on a reflector. It’s usually given in millimeters (mm) or inches (e.g., 130 mm, 8 in).

Why aperture affects brightness (light-gathering)

For extended objects (nebulae, galaxies), image brightness at the eyepiece is mainly controlled by exit pupil (covered below), but aperture still matters because it allows you to use higher magnification while keeping the image reasonably bright. The raw light-gathering ability scales with the area of the aperture:

Light-gathering ∝ aperture²

So going from 100 mm to 200 mm is not “twice as good”—it’s about 4× the light (because (200/100)² = 4).

Why aperture affects resolution (fine detail)

Resolution is the ability to separate fine details (planetary features, tight double stars). In good atmospheric conditions, larger aperture can resolve smaller angular details. A common rule-of-thumb for the diffraction limit is:

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  • Dawes’ limit (arcseconds): 116 / D(mm)
  • Example: 100 mm → ~1.16″; 200 mm → ~0.58″

In practice, the atmosphere (“seeing”) often limits resolution before the telescope does, but aperture still raises the ceiling on what’s possible on steady nights.

The trade-offs: size, cooldown, mount, and cost

  • Bigger aperture = bigger tube (more storage and transport considerations).
  • Heavier optics need a sturdier mount. A shaky mount can erase the benefit of extra aperture.
  • Reflectors with larger mirrors may need more time to reach outdoor temperature for best sharpness.
  • Cost rises quickly because you’re paying for more material, tighter tolerances, and a stronger mount.

Practical comparison example

If you’re comparing a 114 mm reflector vs. a 150 mm reflector:

  • Light-gathering ratio: (150/114)² ≈ 1.73 → the 150 mm gathers ~73% more light.
  • Resolution ratio: 114/150 ≈ 0.76 → the 150 mm can resolve ~24% finer detail (when conditions allow).

2) Focal length and f-ratio: how “wide” or “zoomed” the telescope tends to feel

Focal length: what it is and what it changes

Focal length (FL) is the distance (in mm) over which the telescope brings light to focus. It strongly influences the magnification you get with a given eyepiece:

Magnification = Telescope FL / Eyepiece FL

Example: a 1200 mm telescope with a 25 mm eyepiece gives 1200/25 = 48×. The same eyepiece in a 600 mm telescope gives 600/25 = 24×.

F-ratio (f/number): the “speed” of the optics

F-ratio is focal length divided by aperture:

f-ratio = Telescope FL / Aperture

Example: 200 mm aperture and 1200 mm focal length → f/6. A 100 mm aperture and 900 mm focal length → f/9.

How focal length and f-ratio influence field of view

Two different “fields” matter:

  • True field of view (TFOV): how much sky you see.
  • Apparent field of view (AFOV): a property of the eyepiece (e.g., 50°, 68°, 82°).

A useful approximation:

TFOV ≈ AFOV / Magnification

Step-by-step example:

  • Eyepiece AFOV = 68°
  • Telescope A: 1200 mm FL, eyepiece 24 mm → magnification = 50× → TFOV ≈ 68/50 = 1.36°
  • Telescope B: 600 mm FL, same eyepiece → magnification = 25× → TFOV ≈ 68/25 = 2.72°

Shorter focal length scopes tend to make it easier to get wide, sweeping views with common eyepieces.

How f-ratio affects tolerance to eyepieces and collimation

  • Fast optics (low f/number like f/4–f/6) produce steeper light cones. This tends to be more demanding on eyepiece design; inexpensive eyepieces may show edge distortions more noticeably. Fast Newtonian reflectors are also more sensitive to accurate collimation (mirror alignment).
  • Slow optics (higher f/number like f/8–f/12) are generally more forgiving: budget eyepieces often look better near the edge, and collimation tolerances are looser.

Practical takeaway: if you want to keep eyepiece costs modest and still enjoy clean edges, a slower system can be easier. If you want wide fields and compact tubes, faster systems are attractive, but they reward better eyepieces and careful alignment.

Magnification potential: what focal length does (and doesn’t) guarantee

Longer focal length makes it easy to reach higher magnifications with longer (more comfortable) eyepieces. But aperture and optical quality determine how much magnification is actually usable before the image becomes dim and soft.

3) Exit pupil: the brightness and comfort “dial” you control with eyepiece choice

What exit pupil is

Exit pupil is the diameter of the beam of light leaving the eyepiece. It’s the single most practical way to think about image brightness and viewing comfort.

Two equivalent formulas:

  • Exit pupil (mm) = Aperture (mm) / Magnification
  • Exit pupil (mm) = Eyepiece FL (mm) / f-ratio

Why exit pupil matters

  • Brightness: Larger exit pupil generally gives a brighter view (especially noticeable on deep-sky objects). Too large, and your eye may not accept the full beam, wasting aperture.
  • Comfort and ease of viewing: Very small exit pupils make the view dimmer and can emphasize floaters in your eye; very large exit pupils can make eye placement more finicky depending on eyepiece design.
  • Background sky brightness: Larger exit pupils brighten the sky background too, which can reduce contrast under light pollution.

Step-by-step: compute exit pupil for an eyepiece

Example telescope: 150 mm aperture, 750 mm focal length → f/5.

  • Using a 25 mm eyepiece: Exit pupil = Eyepiece FL / f-ratio = 25/5 = 5 mm
  • Using a 10 mm eyepiece: 10/5 = 2 mm
  • Using a 5 mm eyepiece: 5/5 = 1 mm

Useful exit pupil ranges (practical targets)

Use caseTypical exit pupilWhat it feels like
Wide-field scanning, open clusters, finding objects4–6 mmBright, easy, wide views (sky background also brighter)
General deep-sky viewing (many nebulae/galaxies/clusters)2–3 mmGood balance of brightness and contrast; often a “workhorse” range
Planets, Moon detail, splitting doubles0.5–1.5 mmDimmer but higher scale; steadiness of atmosphere becomes critical
Very high power (only when conditions allow)0.3–0.5 mmOften too dim/soft unless aperture is large and seeing is excellent

Note: your dark-adapted pupil might be ~5–7 mm when young and smaller with age. If your telescope/eyepiece combination produces an exit pupil larger than your eye can open, you won’t get brighter—just effectively reduce the telescope’s working aperture.

4) Practical rules of thumb: magnification limits, marketing traps, and reading spec sheets

Usable magnification: what’s realistic

Magnification is easy to calculate, but not all magnification is useful. Two common guidelines:

  • Rule-of-thumb maximum (optics-limited): about 2× per mm of aperture (or ~50× per inch) under excellent conditions.
  • Typical enjoyable maximum (conditions-limited): often closer to 1× to 1.5× per mm (or ~25× to 40× per inch) depending on seeing, thermal stability, and optical quality.

Example: a 150 mm telescope

  • Optics-limited max: ~300×
  • Commonly useful range on many nights: ~150–225×

Also use exit pupil as a sanity check: if you’re below ~0.5 mm exit pupil, you’re usually in “only if everything is perfect” territory.

Common marketing exaggerations to ignore

  • “675× power!” on small scopes: If the aperture is modest, that number is often achieved only by stacking short eyepieces and Barlows, producing a dim, blurry image. High magnification without resolution is called “empty magnification.”
  • Overemphasis on included accessories: Multiple eyepieces and Barlows bundled with a small, shaky mount don’t compensate for limited aperture or poor stability.
  • Confusing focal length with power: A longer focal length telescope is not automatically “more powerful”; it just reaches a given magnification with a longer eyepiece focal length.

How to read a spec sheet correctly (step-by-step checklist)

  • Step 1: Find aperture (mm). This is your baseline for potential detail and light grasp.
  • Step 2: Note focal length (mm) and compute f-ratio. f = FL / aperture. Use it to anticipate field-of-view flexibility and how picky the scope may be about eyepieces/collimation.
  • Step 3: Estimate realistic magnification range. Start with ~0.5–2× per mm depending on conditions; cross-check with exit pupil targets.
  • Step 4: Evaluate included eyepieces by what they produce. For each eyepiece, compute: Magnification = Telescope FL / Eyepiece FL and Exit pupil = Eyepiece FL / f-ratio. Prefer a spread that hits ~5 mm, ~2–3 mm, and ~1 mm exit pupils rather than chasing extreme power.
  • Step 5: Watch for missing or vague numbers. If aperture isn’t clearly stated, or if “power” is the headline spec, treat it as a red flag and look for a clearer listing.

Quick reference mini-table (common combinations)

TelescopeEyepieceMagnificationExit pupilTypical use
200 mm f/6 (1200 mm FL)30 mm40×5.0 mmWide scanning, large nebulae
200 mm f/6 (1200 mm FL)15 mm80×2.5 mmGeneral deep-sky
200 mm f/6 (1200 mm FL)6 mm200×1.0 mmPlanets, lunar detail
100 mm f/9 (900 mm FL)25 mm36×2.8 mmGeneral viewing, brighter DSOs
100 mm f/9 (900 mm FL)10 mm90×1.1 mmPlanets on steady nights

Now answer the exercise about the content:

If you want a brighter and more comfortable view for wide-field scanning, which eyepiece choice is most likely to help by producing a larger exit pupil (assuming the same telescope)?

You are right! Congratulations, now go to the next page

You missed! Try again.

Exit pupil equals eyepiece focal length divided by f-ratio. With the same telescope, a longer focal length eyepiece gives a larger exit pupil, which generally makes the view brighter and easier for wide-field scanning.

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Refractor Telescopes: Strengths, Limitations, and Best Beginner Setups

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