瑞利分辨极限计算器

θ_min = 1.22·λ / D

Find the minimum resolvable angle for circular-aperture diffraction, θ = 1.22λ/D. For evaluating the resolution limit of telescopes, microscopes and camera lenses.

📐 计算公式
瑞利判据最小分辨角:θ_min = 1.22·λ ÷ D(rad,λ 波长 m、D 圆孔径 m,1.22 为艾里斑一阶零点系数);联动量:µrad = θ×10⁶、角秒 = θ×180/π×3600、度 = θ×180/π。校验:λ、D 两项必填守卫,D 作为分母不得为 0。判据:无固定分级,θ 越小分辨率越高——口径越大或波长越短分辨能力越强。

圆孔衍射的最小可分辨角。

Formula Reference

Item Formula / Note Source / Standard
Rayleigh resolution limitθ = 1.22 λ / D (radians), D = aperture diameterLord Rayleigh (1879)
Airy diskFirst dark-ring angular radius 1.22λ/D from circular-aperture Fraunhofer diffractionAiry (1835) / Hecht, Optics, §10.2
📌 计算说明
  • θ_min = 1.22λ/D。
  • 人眼瞳孔 ~2mm 分辨约 1′。

📐 Physical Constants

Constants used on this page and their authoritative sources, for verification and citation

Constant Value Unit Source
Rayleigh criterion coefficient (circular aperture) 1.2196699… (≈ 1.22) — = first non-zero zero of J₁ divided by π (mathematical constant, exact)
First zero of J₁, j₁,₁ 3.8317059702075125 — Mathematical constant (exact)
One arcminute (1′) 2.908882e-4 rad = π/(180×60), derived from the radian definition

Note: the Rayleigh criterion θ = 1.22λ/D applies to Fraunhofer diffraction by a circular aperture (Airy disc); a slit or square aperture has a different first-zero factor (λ/D for a slit).

📚 深度解析:瑞利分辨判据(角)

💡 常见使用场景

口径 100mm,λ=550nm
θ=1.22λ/D=1.22×550e-9/0.1=6.71e-6rad≈1.39″。两星角距小于此即不可分。
口径 200mm
θ=1.22×550e-9/0.2=3.36e-6rad≈0.69″,分辨力翻倍。

❓ 常见问题(FAQ)

口径越大越清楚?
是:θ∝1/D,口径加倍分辨角减半(受大气视宁度限制时收益递减)。
瑞利与道斯极限?
道斯取 116/D(mm) 角秒,比瑞利 138/D(mm) 略松,常用于目视。