Allicdata Part #: | NSCT817-25LT3G-ND |
Manufacturer Part#: |
NSCT817-25LT3G |
Price: | $ 0.00 |
Product Category: | Discrete Semiconductor Products |
Manufacturer: | ON Semiconductor |
Short Description: | TRANS NPN 45V 0.5A SOT-23 |
More Detail: | Bipolar (BJT) Transistor NPN 45V 500mA 100MHz 225m... |
DataSheet: | NSCT817-25LT3G Datasheet/PDF |
Quantity: | 1000 |
1 +: | 0.00000 |
Series: | -- |
Packaging: | Tape & Reel (TR) |
Part Status: | Obsolete |
Transistor Type: | NPN |
Current - Collector (Ic) (Max): | 500mA |
Voltage - Collector Emitter Breakdown (Max): | 45V |
Vce Saturation (Max) @ Ib, Ic: | 700mV @ 50mA, 500mA |
Current - Collector Cutoff (Max): | 100nA (ICBO) |
DC Current Gain (hFE) (Min) @ Ic, Vce: | 160 @ 100mA, 1V |
Power - Max: | 225mW |
Frequency - Transition: | 100MHz |
Operating Temperature: | -55°C ~ 150°C (TJ) |
Mounting Type: | Surface Mount |
Package / Case: | TO-236-3, SC-59, SOT-23-3 |
Supplier Device Package: | SOT-23-3 (TO-236) |
Base Part Number: | NSCT817 |
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A bipolar junction transistor (BJT) is a three-terminal semiconductor device, consisting of two p-n junction diodes connected together. NSCT817-25LT3G is a single bipolar junction transistor, also known as an NPN transistor, with a 1-amp collector current, a 200-volt collector-emitter voltage and a 1 watt power dissipation. It has three terminals, the base (B), the collector (C) and the emitter (E).
The NSCT817-25LT3G is used for various applications, including switching, amplifying and oscillatory circuits. In addition, it can be used as a booster for power supplies, and for voltage amplifiers and level detectors which are used in many electronic circuits.
The NSCT817-25LT3G has a low saturation voltage, which allows it to work at a high frequency and produces an output stream with minimal distortion. This allows it to be used in a variety of applications, including audio amplifiers, radio receivers, video amplifiers and television receivers.
The working principle of the NSCT817-25LT3G is based on the operation of a p-n junction diode, which is the fundamental building block of a BJT. The base (B) and the emitter (E) are the two p-n junction diodes connected together. The collector (C) is connected to the emitter (E) in order to collect the charges emitted by the emitter.
When a voltage is applied to the base and emitter, a large number of minority carriers are injected in the base region, which creates an access region between the emitter and the collector. This access region allows the collector to collect the minority carriers (electrons or holes) emitted by the emitter.
As the current through the transistor increases, the voltage across the collector and emitter will increase, creating a larger access region and allowing more carriers to cross the emitter-collector gap, thus increasing the current. This is known as the current gain of the transistor. As the current increases, the collector-emitter voltage (VCE) will decrease. This is known as the voltage gain of the transistor.
The power handling capability of the NSCT817-25LT3G is also dependent on the current gain and voltage gain, since the power the transistor can handle is directly proportional to the current and voltage of its input and output signals. This means that the higher the current gain and voltage gain of the transistor, the higher the power handling capability.
In conclusion, the NSCT817-25LT3G is a single bipolar junction transistor with a 1-amp collector current, a 200-volt collector-emitter voltage and a 1 watt power dissipation. It is used for various applications, including switching, amplifying and oscillatory circuits. The working principle of the NSCT817-25LT3G is based on the operation of a p-n junction diode, and its power handling capability is dependent on its current and voltage gains.
The specific data is subject to PDF, and the above content is for reference
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