Reading Field Curves For Heating Devices; High Density (N) Optics: Bcl 500 I \ Bcl 501 I Sn 102 H; Figure 5.18: "High Density" Reading Field Curve For Line Scanner With Heating (Without Deflection Mirror) - Leuze electronic BCL500i Technical Description

Hide thumbs Also See for BCL500i:
Table of Contents

Advertisement

Specifications
5.7

Reading field curves for heating devices

The reading field curves of the heating devices differ to some extent from the normal reading
curves due to the optics heating and are somewhat reduced in the reading field width as well
as in the reading field height!
• The maximum opening angle for all oscillating and deflection mirror devices
(BCL 500
• In addition, the maximum swivel range for all oscillating mirror devices
(BCL 500
deflection mirror models (BCL 500
itation.
• The reading field curves and opening angles are unchanged for all line scanners with
heating (BCL 500
For details, please refer to the following reading field curves for the heating devices.
5.7.1
High Density (N) Optics: BCL 500
400
300
200
100
-100
-200
-300
-400
-100
Figure 5.18: "High Density" reading field curve for line scanner with heating
The reading field curve applies for the reading conditions stated in table 5.9.
52
i
i
\ BCL 501
...100 H) is reduced to ±28° (without heating = ±30°).
i
i
\ BCL 501
O...100 H) is reduced to ±12° (without heating = ±20°). The
i
\ BCL 501
BCL 500/501/504/508
0
100
200
300
Read distance [mm]
(without deflection mirror)
BCL 500
i
i
\ BCL 501
S...100 H) are not affected by this lim-
i
S...102 H), .
i
\ BCL 501
i
SN 102 H
i
SN 102 H
400
500
600
i
i
\ BCL 501
m = 0,25
m = 0,3
m = 0,35
m = 0,5
700
800
900
1000
Leuze electronic

Advertisement

Table of Contents
loading

This manual is also suitable for:

Bcl501i

Table of Contents