Datasheet

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140
800 & 1000 Series
Tubular High Energy Bulk Ceramic
DIMENSIONS
(in.)
C C
Series A B (SP & AS) (A) D
884 SP 2.0 0.50 0.22 – 0.25
885 SP, AS, & A 2.5 0.75 0.50 N/A* 0.50
886 SP, AS, & A 5.0 0.75 0.50 N/A* 0.62
887 SP, AS, & A 6.0 1.00 0.75 0.5 0.50
888 SP, AS, & A 8.0 1.00 0.75 0.5 0.88
889 SP, AS, & A 12.0 1.00 0.75 0.5 0.88
890 SP, AS & A 18.0 1.00 0.75 0.5 0.88
891 SP 18.0 2.00 1.50 – 1.00
892 SP 24.0 2.00 1.50 – 1.00
1026 AS 6.0 1.50 1.00 – 0.50
1028 AS 8.0 1.50 1.00 – 0.88
1032 AS 12.0 1.50 1.00 – 0.88
1038 AS 18.0 1.50 1.00 – 0.88
1044 AS 24.0 1.50 1.00 – 0.88
Special sizes are available. Consult factory.
*885 and 886 in type A material are solid rods
A ±1/16
D ±1/18
Metallized Ends
B ±1/32
C Nom.
CHARACTERISTICS
TERMINATION OPTIONS
Derating
Mounting Clips
Surface Temperature
Ambient Temperature (°C)
SP
100
40
80
20
60
0
% Rated Power
40°
300 400100 2000
350° 230°
AS & A
% Rated Power
SP
AS
Temperature Rise (°C)
200
100
350
150
50
250
300
0
0 20 40 60 80 100 120
Power ratings are
based on maximum
allowable surface tem-
perature in still air at
40°C ambient tempera-
ture.
Curve is typical for
resistor midpoint with
horizontal orientation in
still air.
Electrical connection to the
resistive bodies of resis-
tors is made by metal end
bands. The standard metal is
aluminum for Type SP, silver
for Type AS and nickel for
Type A. Special terminations
of brass, copper or soldered
ends are also available.
In most cases, connections to
the resistors may be made by
using these stock clips.
Material: Beryllium Copper
Finish: Electro Tin Plate
C max.
T ±.001"
D ±0.015"
A max.
B
W
F ±0.003"
V ±0.005"
V ±0.005"
E
V
Resistor Resistor
Part No. series OD Holes A B C D E F T V W (in.)
35370 884 1/2 1 0.620 0.090 0.560 0.500 N/A 0.093 0.020 0.188 0.375
35267 885, 886 3/4 1 0.940 0.155 0.830 0.750 N/A 0.144 0.020 0.312 0.625
35268 887 - 890 1 2 1.230 0.170 1.070 1.000 0.320 0.128 0.024 0.156 0.625
35371 891, 892 1 1/2 2 1.650 0.100 1.650 1.500 0.925 0.103 0.032 0.250 0.500
35269 1026 - 1044 2 2 2.375 0.544 1.080 2.000 0.375 0.188 0.043 0.375 0.750