Allicdata Part #: | NSL-4132-ND |
Manufacturer Part#: |
NSL-4132 |
Price: | $ 0.39 |
Product Category: | Sensors, Transducers |
Manufacturer: | Luna Optoelectronics |
Short Description: | PHOTOCELL CDS 500OHM TO-18 |
More Detail: | CDS Cell 550nm 18 ~ 42 kOhms @ 10 lux |
DataSheet: | NSL-4132 Datasheet/PDF |
Quantity: | 1000 |
3250 +: | $ 0.34373 |
Series: | -- |
Part Status: | Active |
Wavelength: | 550nm |
Voltage - Max: | 80Vpk |
Cell Resistance (Min) @ Dark: | 1.8 MOhms @ 5s |
Cell Resistance @ Illuminance: | 18 ~ 42 kOhms @ 10 lux |
Operating Temperature: | -60°C ~ 75°C (TA) |
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Optical Sensors, such as Photo Detectors, are used in a variety of fields and applications depending on what they are intended to measure. One of these is the CdS (Cadmium Sulfide) cell, which is used in the NSL-4132 application field and working principle. CdS cells have wide applications in light-sensitive switching circuits, control circuits, signal transmission, communication, security systems, and environmental monitoring.
The NSL-4132 Optical Intensity Transducer utilizes CdS cells and its application field and working principle are both fairly complex. To start with, the basic material component of the NSL-4132 are two CdS Cells, which act as photodetectors. The CdS Cells form the core of the device, and sense the light intensity, providing a direct output of electrical current through the light intensity. The device is connected to a circuit, with power supply operated by two batteries for energy. The circuit is composed of a current source, a control circuit, an amplifier, and a frequency-controlled switching device.
When exposed to light, the anode side negative potential increases and the cathode side positive potential decreases. This potential difference causes electrons from the anode side to be released, and then flows to the cathode side because of the electric field between the two, which generates current, thus forming an electric signal.
The resistance of the CdS cell varies according to the level of light intensity, causing the electric current generated by the device to vary. This current is then amplified by the amplifier circuit, and power is supplied to the switching device, which controls the frequency of the output current. The output current can then be measured by a voltage reader, allowing comparison of light intensity values and readouts from the device.
The NSL-4132 utilizes the CdS cell for direct optical power determination without any additional components or additional calibrations. Its applications are also quite wide ranging, including, but not limited to, automotive lighting and dark room illumination, motion detectors and proximity sensors, light dependent resistor (LDR) circuits, photocopiers, and flash photography.
The working principle of the NSL-4132 Optical Intensity Transducer is quite easy to understand and its use is widespread. The transducer works by detecting changes of light intensity using the CdS cells and calculating the current flowing through the device and providing an output that can be measured easily. This is an effective way to detect and measure light intensity and further allows for the measurement of light transmission during certain situations.
In conclusion, the NSL-4132 application field and working principle is easy to understand, and it utilizes CdS cells to provide a direct output of electrical current through the light intensity. Its various applications are also quite wide-ranging and range from automotive lighting and darkroom illumination, to motion detectors and photcopiers. Its use is widespread, and its cost is comparatively quite low – making it a popular choice for many applications in need of optical sensors and detectors.
The specific data is subject to PDF, and the above content is for reference
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