Allicdata Part #: | 2SC4132T100RTR-ND |
Manufacturer Part#: |
2SC4132T100R |
Price: | $ 0.00 |
Product Category: | Discrete Semiconductor Products |
Manufacturer: | ROHM Semiconductor |
Short Description: | TRANS NPN 120V 2A SOT-89 |
More Detail: | Bipolar (BJT) Transistor NPN 120V 2A 80MHz 2W Surf... |
DataSheet: | 2SC4132T100R Datasheet/PDF |
Quantity: | 1000 |
Series: | -- |
Packaging: | Tape & Reel (TR) |
Part Status: | Not For New Designs |
Transistor Type: | NPN |
Current - Collector (Ic) (Max): | 2A |
Voltage - Collector Emitter Breakdown (Max): | 120V |
Vce Saturation (Max) @ Ib, Ic: | 2V @ 100mA, 1A |
Current - Collector Cutoff (Max): | 1µA (ICBO) |
DC Current Gain (hFE) (Min) @ Ic, Vce: | 180 @ 100mA, 5V |
Power - Max: | 2W |
Frequency - Transition: | 80MHz |
Operating Temperature: | 150°C (TJ) |
Mounting Type: | Surface Mount |
Package / Case: | TO-243AA |
Supplier Device Package: | MPT3 |
Base Part Number: | 2SC4132 |
Due to market price fluctuations, if you need to purchase or consult the price. You can contact us or emial to us: sales@allicdata.com
2SC4132T100R, also known as NPN Silicon High-Frequency Transistor, is a type of Bipolar (BJT) and Single Transistor. This transistor is especially useful for applications which require high-frequency operation due to its small signal performance and high breakdown voltage.Given its outstanding features, 2SC4132T100R has a wide range of practical applications, including usage in signal amplification equipment, low-loss switching circuits, and low power mixer stages. It is also used in FM transmitters, class A & B amplifiers, and television signal processing.The working principle of the 2SC4132T100R transistors can be understood in a simple manner. When a small signal is applied to the base input which is connected to the emitter, the resulting small current is amplified by the collector current which flows through the collector-emitter junction. As the collector current increases, it causes a proportional increase in voltage across the collector-emitter junction that is the output voltage. This process is known as base-emitter biasing, which is the fundamental principle behind the operation of a BJT transistor.In order to ensure the correct functioning of a 2SC4132T100R, it is important to note that the current but into the transistor should not exceed the maximum collector current rating. In addition, the input current should lie within the allowable range changes. Moreover, the voltage at the base should be maintained within the specified rating.In addition to the base-emitter biasing that form the basis of its functionality, the 2SC4132T100R also utilizes two other mechanisms, namely: collector-emitter saturation and collector-emitter cut-off. The first mechanism involves the application of bias voltage to the collector-emitter junction when the base current becomes larger than a certain value. This results in the current to decrease slightly before it suddenly shoots up and saturates at a particular level. The second mechanism takes place in a reverse fashion each time the base current is reduced below a certain threshold, causing the current to cut-off.Finally, it is also important to consider the temperature rating when using the 2SC4132T100R transistors. This is because the operating temperature can significantly affect the collector-emitter voltage and the collector-emitter saturation voltage. Specifically, the temperature of the transistor can significantly reduce by lowering the collector-emitter voltage and increase by raising the saturation voltage.Overall, 2SC4132T100R transistors are ideal for a wide range of applications due to their small signal performance, large breakdown voltage, and the fact that they are able to operate at higher frequencies than other transistors. The working principle of these transistors can also be understood in a simple manner which involves base-emitter biasing, collector-emitter saturation, and collector-emitter cut-off. It is also important to keep in mind the temperature rating as this can have a major impact on the transistors’ performance. With all this in mind, the 2SC4132T100R transistors are well-suited for use in a number of industrial and commercial applications.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
2SC4212H | Panasonic El... | 0.0 $ | 1000 | TRANS NPN 300V 0.2A TO-12... |
2SC4953 | Panasonic El... | 0.0 $ | 1000 | TRANS NPN 400V 3A TO-220D... |
2SC4208ARA | Panasonic El... | 0.0 $ | 1000 | TRANS NPN 50V 0.5A TO-92N... |
2SC43910RA | Panasonic El... | 0.0 $ | 1000 | TRANS NPN 80V 1A MT-2Bipo... |
2SC4015TV2N | ROHM Semicon... | 0.0 $ | 1000 | TRANS NPN 300V 0.1A ATVBi... |
2SC4620TV2P | ROHM Semicon... | 0.0 $ | 1000 | TRANS NPN 400V 0.1A ATVBi... |
2SC4081RT1 | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 50V 0.1A SC70Bi... |
2SC4793(F,M) | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 230V 1A TO220NI... |
2SC4488T-AN | ON Semicondu... | -- | 1000 | TRANS NPN 100V 1A NMPBipo... |
2SC4487T-ANX | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 50V 0.3A NMPBip... |
2SC4488S-YMH-AN | ON Semicondu... | 0.0 $ | 1000 | TRANS BIPO NMPBipolar (BJ... |
2SC4488T-YMH-AN | ON Semicondu... | 0.0 $ | 1000 | TRANS BIPO NMPBipolar (BJ... |
2SC4604,F(J | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 3A 50V TO226-3B... |
2SC4604,T6F(J | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 3A 50V TO226-3B... |
2SC4604,T6F(M | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 3A 50V TO226-3B... |
2SC4682,T6CSF(J | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 3A 15V TO226-3B... |
2SC4682,T6F(J | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 3A 15V TO226-3B... |
2SC4793(LBSAN,F,M) | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 1A 230V TO220-3... |
2SC4793(PAIO,F,M) | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 1A 230V TO220-3... |
2SC4793,F(J | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 1A 230V TO220-3... |
2SC4793,HFEF(J | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 1A 230V TO220-3... |
2SC4793,HFEF(M | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 1A 230V TO220-3... |
2SC4793,NSEIKIF(J | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 1A 230V TO220-3... |
2SC4793,TOA1F(J | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 1A 230V TO220-3... |
2SC4793,WNLF(J | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 1A 230V TO220-3... |
2SC4793,YHF(J | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 1A 230V TO220-3... |
2SC4793,YHF(M | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 1A 230V TO220-3... |
2SC4881(CANO,F,M) | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 5A 50V TO220-3B... |
2SC4881,LS1SUMIF(M | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 5A 50V TO220-3B... |
2SC4935-Y,Q(J | Toshiba Semi... | 0.0 $ | 1000 | TRANS NPN 3A 50V TO220-3B... |
2SC4116-BL,LF | Toshiba Semi... | 0.02 $ | 1000 | TRANS NPN 50V 0.15A USMBi... |
2SC4617EBTLP | ROHM Semicon... | -- | 1000 | TRANS NPN 50V 0.15A EMT3B... |
2SC4211-7-TL-E | ON Semicondu... | 0.08 $ | 1000 | TRANS NPN 50V 0.15A SOT-3... |
2SC4132T100R | ROHM Semicon... | -- | 1000 | TRANS NPN 120V 2A SOT-89B... |
2SC4135T-TL-E | ON Semicondu... | 0.18 $ | 1000 | TRANS NPN 100V 2A TP-FABi... |
2SC4672T100P | ROHM Semicon... | -- | 1000 | TRANS NPN 50V 2A SOT-89Bi... |
2SC4134S-E | ON Semicondu... | 0.22 $ | 1000 | TRANS NPN 100V 1A TPBipol... |
2SC4027T-E | ON Semicondu... | 0.22 $ | 1000 | TRANS NPN 160V 1.5A TPBip... |
2SC4027S-TL-H | ON Semicondu... | 0.22 $ | 1000 | TRANS NPN 160V 1.5A TP-FA... |
2SC4132T100P | ROHM Semicon... | 0.22 $ | 1000 | TRANS NPN 120V 2A SOT89Bi... |
GENERAL-PURPOSE TRANSISTORBipolar (BJT) ...
TRANS PNP DARL 30A 120V DIEBipolar (BJT)...
TRANS PNP DARLINGTON DIEBipolar (BJT) Tr...
TRANS GENERAL PURPOSE TO-218Bipolar (BJT...
TRANS PNP 140V 1ABipolar (BJT) Transisto...
TRANS NPN 700V 3A I2PAKBipolar (BJT) Tra...