|
|
|
BL |
= |
ß + ØL (0.3048) |
|
BL |
= |
Beam Diameter (mm) at distance
L |
|
ß |
= |
Increase in Beam Diameter |
|
|
= |
Beam Diameter (mm) x Expander
Power |
|
Ø |
= |
Decrease in Beam
Divergence |
|
|
= |
Beam Divergence (mrad) Expander
Power |
|
L |
= |
distance
(ft.) |
This equation is an approximation for the collimated output beam size at a given distance.
In addition, an expanded
beam can yield smaller spot sizes when used in combination with additional
focusing
optics. This is very useful in focusing optimization. however, many
applications simply require a larger continuous
beam.
The beam
expander power (MP) is equal to the ratio of the effective focal length (EFL) of
the objective lens
to the effective focal length of the entrance optic. The
physical separation between the objective lens and entrance
optic is equal
to the sum of their back focal lengths (BFL).
DiOptika’s beam expanders are of
the Galilean type. The advantages of the Galilean design over the Keplerian
is
that it contains no internal focal point therefore reducing the
length. In addition to improving
beam collimation,
DiOptika’s beam expanders can also be used to focus laser
beams.