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Ideal Two-Lens Laser Beam Expansion

Relate focal lengths, beam diameter and full-angle divergence for an ideal beam expander.

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Calculator inputs

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How to use this calculator

  1. Enter the known values in the units shown. Results update as you type.
  2. Where results are editable, change one to solve backwards. Lock a value to hold it fixed.
  3. Use the worked example to check the method. Reset restores the starting fields.

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Formula and method

magnification power = 5.0000; magnification = 0.20000. This worked example uses the displayed units and declared assumptions.

magnification_power = focal_length_objective/(type *focal_length_image); magnification = 1/magnification_power; output_diameter=input_diameter*magnification_power; output_divergence = input_divergence/magnification_power; diameter_at_distance_L = output_diameter + 2*L*tan(output_divergence/2)

Worked example

Enter these known values and leave the other values blank.

Design
1
Image lens' focal length (f==ɪ==)
20 mm
Objective lens' focal length (f==O==)
100 mm
Input diameter (D==ɪ==)
2 mm
Input divergence (Θ==ɪ==)
5 mrad
Distance from the expander (L)
10 m
Magnification (m)
0.2
Magnifying power (MP)
5 X
Output diameter (D==O==)
10 mm
Output divergence (Θ==O==)
1 mrad
Diameter at distance (D==L==)
20 mm

Assumptions and limitations

  • This paraxial two-lens model assumes a collimated input and ideal aligned lenses. Expansion ratio is objective focal length divided by the signed input focal length times the selected lens type.
  • Divergence is the full included angle. Propagation uses straight edge rays, D(L)=D0+2L tan(theta/2); it is not Gaussian-beam waist propagation and does not include diffraction or aberration.

Common questions

What assumptions apply?

This paraxial two-lens model assumes a collimated input and ideal aligned lenses. Expansion ratio is objective focal length divided by the signed input focal length times the selected lens type.

Which unknowns can I solve?

Editable controls preserve the supported captured inverse branches. Clear the desired unknown and provide enough independent known quantities; singular or underdetermined inverses may remain incomplete.

References

Declare divergence as the full included angular width. Two symmetric edge rays each travel at theta/2, so diameter grows by 2 L tan(theta/2), with each captured inverse updated consistently. Expansion ratio and inverse divergence relation retain their paraxial lens assumptions.

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