Resolving Power Calculator
Resolving power sets the limit on how fine a detail an optical instrument can distinguish. It is set by diffraction — larger apertures and shorter wavelengths give better resolution.
Formula & Reference
| Variable | Symbol | Formula | Units |
|---|---|---|---|
| Angular Resolution | θ | θ = 1.22λ/D | rad |
| Min Resolution (Microscope) | d | d = 1.22λ/(2 NA) | m |
| Aperture | D | Diameter of lens/mirror | m |
| Numerical Aperture | NA | n sin(α) | — |
Step-by-Step Examples
Pupil D=5 mm, lambda=550 nm.
- theta = 1.22 * 550e-9 / 0.005 = 1.34e-4 rad = 27.6 arcsec
D=2.4 m, lambda=550 nm.
- theta = 1.22 * 550e-9 / 2.4 = 2.8e-7 rad = 0.058 arcsec
D=1 cm objective, NA=0.65, lambda=550 nm.
- d = 1.22 * 550e-9 / (2*0.65) = 516 nm = 0.52 um
Real-World Applications
Common Mistakes to Avoid
Other criteria exist (Sparrow, Abbe). Rayleigh criterion (first minimum of one coincides with center of other) is most common.
In a medium with n>1, effective wavelength is lambda/n. This is why oil-immersion microscopes improve resolution.
Not always — atmospheric seeing limits ground-based telescopes. Adaptive optics corrects this; space avoids it.
Frequently Asked Questions
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