BC560CTA Discrete Semiconductor Products |
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Allicdata Part #: | BC560CTATB-ND |
Manufacturer Part#: |
BC560CTA |
Price: | $ 0.03 |
Product Category: | Discrete Semiconductor Products |
Manufacturer: | ON Semiconductor |
Short Description: | TRANS PNP 45V 0.1A TO-92 |
More Detail: | Bipolar (BJT) Transistor PNP 45V 100mA 150MHz 500m... |
DataSheet: | BC560CTA Datasheet/PDF |
Quantity: | 16000 |
2000 +: | $ 0.02663 |
6000 +: | $ 0.02315 |
10000 +: | $ 0.01968 |
50000 +: | $ 0.01736 |
100000 +: | $ 0.01544 |
Series: | -- |
Packaging: | Tape & Box (TB) |
Part Status: | Active |
Transistor Type: | PNP |
Current - Collector (Ic) (Max): | 100mA |
Voltage - Collector Emitter Breakdown (Max): | 45V |
Vce Saturation (Max) @ Ib, Ic: | 650mV @ 5mA, 100mA |
Current - Collector Cutoff (Max): | 15nA (ICBO) |
DC Current Gain (hFE) (Min) @ Ic, Vce: | 420 @ 2mA, 5V |
Power - Max: | 500mW |
Frequency - Transition: | 150MHz |
Operating Temperature: | 150°C (TJ) |
Mounting Type: | Through Hole |
Package / Case: | TO-226-3, TO-92-3 (TO-226AA) (Formed Leads) |
Supplier Device Package: | TO-92-3 |
Base Part Number: | BC560 |
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BC560CTA is an NPN silicon transistor commonly used for general purpose amplification, switching and preamplification applications. It is mainly used in consumer electronic equipment, automotive electronics, and computer peripherals. The BC560CTA has a high voltage gain, low noise, and a low collector-emitter saturation voltage making it well suited for many applications.
The active region of the BC560CTA consists of a P-type semiconductor region sandwiched between two N-type semiconductor regions. In the BC560CTA, the N-type regions are the emitter and collector regions, while the P-type region is the base region. In the base region, two N-type impurity atoms interact with a single P-type impurity atom. When a voltage is applied to the base-emitter junction, electrons from the N-type region move over the P-type region, which forms a semiconductor bridge.
With the application of a voltage across the base-emitter junction, electrons start flowing from the N-type region to the P-type region, creating an avalanche effect. As more electrons start flowing, the base current increases exponentially. The number of electrons amplified due to the avalanche effect is called the current gain. The current gain of the BC560CTA is typically in the range of 300 to 700, which is enough to amplify electronic signals in applications such as switching, testing, and sensing.
When a voltage is applied to the collector-emitter junction and a current flows, the BC560CTA acts as an amplifier. The collector-emitter voltage is proportional to the base current, with changes in the base current resulting in changes in the voltage. The voltage gain is approximately the same as the current gain. This makes the BC560CTA a good choice for applications such as amplifying weak signals and controlling power output in transistor circuits.
Also, the BC560CTA has a low collector-emitter saturation voltage. This is important in applications such as analog audio amplification, where the collector-emitter saturation voltage must remain low to prevent distortion of the audio signal. The low saturation voltage also helps reduce power consumption and increases the efficiency of the device.
Due to its low noise, high voltage gain, low collector-emitter saturation voltage, and high current gain, the BC560CTA is ideal for applications such as audio amplification, switching, sensing, and testing. Its low noise and wide range of currents make it suitable for a variety of consumer electronic applications.
The specific data is subject to PDF, and the above content is for reference
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