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SDP8601 - Optoschmitt Detector

Download the SDP8601 datasheet PDF. This datasheet also covers the SDP8600 variant, as both devices belong to the same optoschmitt detector family and are provided as variant models within a single manufacturer datasheet.

Description

The SDP86XX series is a family of single chip Optoschmitt IC detectors molded in a side-looking black plastic package to minimize the effect of visible ambient light.

Features

  • Side-looking plastic package.
  • 55¡ (nominal) acceptance angle.
  • Wide sensitivity ranges.
  • TTL/LSTTL/CMOS compatible.
  • Buffer (SDP8600/8601/8602) or inverting (SDP8610/8611/8612) logic available.
  • Three different lead spacing arrangements.
  • Mechanically and spectrally matched to SEP8506 and SEP8706 infrared emitting diodes.

📥 Download Datasheet

Note: The manufacturer provides a single datasheet file (SDP8600_ETC.pdf) that lists specifications for multiple related part numbers.

Datasheet Details

Part number SDP8601
Manufacturer Honeywell
File Size 562.74 KB
Description Optoschmitt Detector
Datasheet download datasheet SDP8601 Datasheet

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Full PDF Text Transcription (Reference)

The following content is an automatically extracted verbatim text from the original manufacturer datasheet and is provided for reference purposes only.

View original datasheet text
SDP86XX Optoschmitt Detector FEATURES • Side-looking plastic package • 55¡ (nominal) acceptance angle • Wide sensitivity ranges • TTL/LSTTL/CMOS compatible • Buffer (SDP8600/8601/8602) or inverting (SDP8610/8611/8612) logic available • Three different lead spacing arrangements • Mechanically and spectrally matched to SEP8506 and SEP8706 infrared emitting diodes DESCRIPTION The SDP86XX series is a family of single chip Optoschmitt IC detectors molded in a side-looking black plastic package to minimize the effect of visible ambient light. The photodetector consists of a photodiode, amplifier, voltage regulator, Schmitt trigger and an NPN output transistor with a 10 kì (nominal) pull-up resistor. Output rise and fall times are independent of the rate of change of incident light.
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