Allicdata Part #: | KSC2982BTF-ND |
Manufacturer Part#: |
KSC2982BTF |
Price: | $ 0.00 |
Product Category: | Discrete Semiconductor Products |
Manufacturer: | ON Semiconductor |
Short Description: | TRANS NPN 10V 2A SOT-89 |
More Detail: | Bipolar (BJT) Transistor NPN 10V 2A 150MHz 500mW S... |
DataSheet: | KSC2982BTF Datasheet/PDF |
Quantity: | 1000 |
Series: | -- |
Packaging: | Tape & Reel (TR) |
Part Status: | Obsolete |
Transistor Type: | NPN |
Current - Collector (Ic) (Max): | 2A |
Voltage - Collector Emitter Breakdown (Max): | 10V |
Vce Saturation (Max) @ Ib, Ic: | 500mV @ 50mA, 2A |
Current - Collector Cutoff (Max): | 100nA (ICBO) |
DC Current Gain (hFE) (Min) @ Ic, Vce: | 200 @ 500mA, 1V |
Power - Max: | 500mW |
Frequency - Transition: | 150MHz |
Operating Temperature: | 150°C (TJ) |
Mounting Type: | Surface Mount |
Package / Case: | TO-243AA |
Supplier Device Package: | SOT-89-3 |
Base Part Number: | KSC2982 |
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KSC2982BTF transistors are designed for use in Voltage Regulator Modules (VRMs) for computing and graphics processing applications. They are available in a variety of packages, including a three-terminal package with top-side configuration for use in footprints such as a BGA (ball grid array) or an LGA (land grid array) socket. The KSC2982BTF has a maximum operating temperature of 125°C and a maximum breakdown voltage of 85V.
A KSC2982BTF transistor is a bipolar junction transistor (BJT). BJTs have three terminals: an emitter, a collector, and a base. The emitter and collector are the heavily doped regions, which form the junction of the transistor. The base is the lightly doped region, which is responsible for controlling the flow of current between the emitter and the collector. The base is connected to the control voltage source VCE.
When a control voltage VCE is applied at the base, the base-emitter junction becomes forward-biased and allows current to flow from the emitter to the base. This process is known as the Emitter Follower configuration. The resulting current flow is known as the collector current and is given by:
Where:
β = hFE (current gain)
VBE = base-emitter voltage
VCE = control voltage
IB = base current
Thus, when a base voltage VBE is applied, the collector current is determined by the ratio of the current gain β and the sum of the base voltage VBE and the control voltage VCE. For example, for an applied VBE of 0.7V and a current gain of 100, the collector current will be:
IC = 100*(0.7V + VCE)
The voltage drop across the base-emitter junction is VBE and is typically 0.7V. The voltage drop across the collector-emitter junction is VCE and is typically between 5 and 10V. The current gain β of a KSC2982BTF transistor can range from 10 to 100, depending on the applied VCE.
The KSC2982BTF can be used in many applications, such as voltage regulation modules (VRMs) and DC-DC converters. It can also be used as an amplifier, as a switch, or as a voltage regulator, depending on the configuration of the circuit.
The KSC2982BTF has good thermal characteristics, allowing higher operating temperatures with lower thermal resistance than other types of transistors. It also has a very low leakage current and is capable of high current gains. Additionally, the KSC2982BTF is highly reliable and has a very low saturation voltage.
In conclusion, the KSC2982BTF is a bipolar junction transistor (BJT) designed for high-current applications, such as DC-DC converters and voltage regulator modules. The KSC2982BTF has a high current gain, excellent thermal characteristics, low saturation voltage, and low leakage current, making it ideal for a wide range of applications.
The specific data is subject to PDF, and the above content is for reference
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