Formula Used
A common microscope definition of one Airy unit at the pinhole plane is the Airy-disk diameter in the image plane:
d1AU = 1.22 · λ · M / NA
- d1AU is the 1 AU pinhole diameter (µm).
- λ is the emission wavelength (µm).
- M is the total magnification to the pinhole plane.
- NA is the objective numerical aperture.
For a chosen Airy-unit setting, the recommended pinhole diameter is:
d = AU · d1AU.
For a known pinhole diameter, the equivalent Airy units are:
AU = d / d1AU.
How to Use This Calculator
- Select a mode: compute diameter or compute Airy units.
- Enter emission wavelength, NA, and total magnification.
- Enter either Airy units or pinhole diameter, depending on mode.
- Press Calculate to see results above the form.
- Use the CSV/PDF buttons to save your setup notes.
Professional Article
1) Why pinhole size matters in confocal imaging
In a confocal microscope, the pinhole rejects out‑of‑focus fluorescence before it reaches the detector. A smaller pinhole increases optical sectioning and contrast, but it also reduces detected photons and can raise shot noise. The practical goal is to balance axial discrimination with usable signal for your sample.
2) Airy units as a standard reference
Many systems express pinhole size in Airy units (AU), where 1 AU is tied to the diffraction pattern of the objective. Using AU helps compare different objectives and wavelengths. Typical starting points are 1.0 AU for general imaging and 0.8 AU for thinner optical sections when signal permits.
3) The role of wavelength in the recommended diameter
Emission wavelength directly affects the Airy disk size. Longer wavelengths create larger diffraction patterns, so 1 AU becomes larger. For example, moving from 520 nm to 640 nm can increase the 1 AU diameter by roughly 20–30% for similar NA and magnification. Multi‑color imaging often benefits from choosing a wavelength‑aware setting.
4) Numerical aperture and resolution tradeoffs
Higher NA objectives form smaller Airy disks and improve lateral and axial resolution. Because 1 AU scales with
1/NA, switching from NA 1.00 to NA 1.40 reduces the 1 AU diameter by about 29% for the same wavelength and
magnification. High‑NA lenses therefore reach strong sectioning at smaller pinhole openings.
5) Magnification and relay optics considerations
The magnification term represents the total imaging scale to the pinhole plane, which can include intermediate optics, scan lenses, and tube lenses. If your system uses additional relay magnification, the effective M increases and the required physical pinhole diameter for 1 AU increases proportionally. Documenting the full optical train improves repeatability across instruments.
6) Practical operating ranges and signal planning
A common operational range is 0.8–1.2 AU. Below ~0.7 AU, photomultiplier‑based systems may require more laser power or longer dwell time, increasing photobleaching risk. Above ~1.5 AU, optical sectioning weakens and background rises, which can reduce effective contrast in thick specimens.
7) Sampling, pixel size, and downstream quantification
Pinhole choice interacts with pixel size and z‑step. Tight pinholes improve axial confinement, but you must still sample adequately to avoid losing detail. As a rule of thumb, use Nyquist‑friendly pixel sizes and z‑steps that capture the expected point spread function while keeping photon budgets realistic for quantitative comparisons.
8) Best practices for consistent reporting
For reproducible imaging, record wavelength, objective NA, total magnification, and pinhole setting in both AU and micrometers. When switching fluorophores, recompute 1 AU using the emission channel. This calculator helps standardize those choices and provides export files for lab notebooks and instrument logs.
FAQs
1) What is a good default pinhole setting?
Start near 1.0 AU for general confocal imaging. It usually balances optical sectioning and signal, especially for thin samples or moderate brightness.
2) Should I use excitation or emission wavelength?
Most confocal systems define 1 AU using the emission wavelength for the selected detection channel, since the detected fluorescence determines the diffraction pattern at the pinhole.
3) What happens if I close the pinhole too much?
Optical sectioning improves, but photon counts drop. You may need higher laser power or longer dwell time, which can increase bleaching and phototoxicity.
4) What happens if I open the pinhole too far?
Signal increases, but out‑of‑focus light rises. Background can reduce contrast and make axial features appear thicker than they are.
5) Why does NA change the recommended diameter?
Higher NA produces a smaller Airy disk. Because 1 AU scales with 1/NA, increasing NA reduces the physical pinhole diameter needed for the same AU setting.
6) Can I use one pinhole size for multicolor imaging?
You can, but it may not be optimal. Longer emission wavelengths need larger 1 AU diameters. For consistent sectioning, compute AU per channel or select a compromise setting.
7) Does magnification always equal the objective label?
Not always. Many microscopes include relay optics that change the effective magnification at the pinhole plane. Use the total magnification specified by your instrument configuration.
Example Data Table
| Wavelength (nm) | NA | M | Airy Units | 1 AU Diameter (µm) | Recommended Diameter (µm) |
|---|---|---|---|---|---|
| 520 | 1.40 | 60 | 1.0 | 27.2 | 27.2 |
| 640 | 1.30 | 63 | 0.8 | 37.8 | 30.3 |
| 488 | 1.00 | 40 | 1.2 | 23.8 | 28.6 |
Values are illustrative. Your system’s relay optics may change M.