Microscope "Numerical Aperture (NA)": A More Important Parameter Than Magnification

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I. What Is NA? Definition and Principle
1. Core Definition
NA is an indicator measuring the light-gathering ability and resolution of an objective lens, representing "the ability to capture light" — a higher NA means more light collected and clearer imaging (e.g., an NA of 1.4 collects approximately 3 times more light than an NA of 0.8, making it superior for observing weak signals).
2. Calculation Formula and Key Conclusions
Formula: NA = n × sinθ (where n = refractive index of the medium, θ = half-angle of aperture, with a maximum of 90°, and sin90° = 1)
  • Conclusion 1: The higher the medium’s refractive index (n), the higher the upper limit of NA. For example, air (n=1.0) has an NA upper limit of 1.0; oil immersion (n=1.515) has an upper limit of 1.515 — this explains why oil-immersion objectives can have an NA higher than 1.0 and are the first choice for high-resolution observation.​
  • Conclusion 2: The larger the half-angle of aperture (θ, i.e., the wider the objective opening), the higher the NA. High-end objectives expand θ through optimized optical design (e.g., increasing the number of lenses, using special glass materials) to improve NA.​
3. Direct Correlation with Resolution
According to Abbe’s Resolution Formula (proposed by Ernst Abbe in 1873), a microscope’s resolution (d, the minimum distance between two distinguishable adjacent objects) is inversely proportional to NA:
d = 0.61 × λ / NA
(where λ = wavelength of the light source, e.g., the average wavelength of visible light λ=550nm).
This means: With a fixed light source wavelength, a higher NA results in a smaller resolution d, allowing observation of finer details. For example:
  • When observing with visible light (λ=550nm), an objective with NA=0.8 has a resolution d=0.61×550nm /0.8≈421nm;​
  • Under the same wavelength, an objective with NA=1.4 has a resolution d=0.61×550nm /1.4≈240nm;​
  • With oil-immersion medium (n=1.515) and NA=1.5, the resolution can be further improved to d≈0.61×550nm /1.5≈223nm.​
It is evident that doubling the NA (from 0.7 to 1.4) can approximately double the resolution — an effect impossible to achieve by simply increasing magnification. This is the core scientific basis for why NA is more important than magnification.
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II. Three Core Impacts of NA: Resolution, Image Brightness, and Depth of Field
Numerical aperture not only determines resolution but also directly affects image brightness and depth of field (the thickness range of a sample that can be clearly imaged). Together, these three factors determine the practical performance of a microscope.
1. Impact 1: Resolution (Most Critical)
As shown in Abbe’s formula, NA is the "determinant" of resolution. High-NA objectives can distinguish details that low-NA objectives cannot:
  • A 40× objective with NA=0.8 (d≈421nm): Can clearly show the morphology of E. coli (0.5-1μm) but cannot resolve surface flagella (≈20nm in diameter);​
  • A 100× oil-immersion objective with NA=1.4 (d≈240nm): Can observe the distribution of flagella; observing 20nm nanoparticles requires an objective with higher NA and a special light source.​
2. Impact 2: Image Brightness
Image brightness is proportional to the square of NA (brightness ∝ NA²) — doubling the NA quadruples the brightness. This is critical for observing weak signals (e.g., fluorescently labeled low-expression proteins, transparent biological samples):
  • A European hospital used an objective with NA=0.75 to observe fluorescent cells. Insufficient brightness required prolonged exposure, reducing cell viability;​
  • After switching to an objective with NA=1.4, brightness increased by approximately 3.5 times, shortening exposure time and preserving cell viability.​
3. Impact 3: Depth of Field (DOF)
NA is inversely proportional to depth of field — a higher NA results in a smaller DOF:
  • High NA (1.4): Suitable for thin samples or surface details (e.g., chip solder joints); frequent focus adjustment is required for thick samples;​
  • Low NA (0.3): Suitable for thick samples (e.g., ores); can observe multiple layers at once but has lower resolution.
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