2SB1181TLR Allicdata Electronics
Allicdata Part #:

2SB1181TLRTR-ND

Manufacturer Part#:

2SB1181TLR

Price: $ 0.00
Product Category:

Discrete Semiconductor Products

Manufacturer: ROHM Semiconductor
Short Description: TRANS PNP 80V 1A SOT-428
More Detail: Bipolar (BJT) Transistor PNP 80V 1A 100MHz 10W Sur...
DataSheet: 2SB1181TLR datasheet2SB1181TLR Datasheet/PDF
Quantity: 1000
Stock 1000Can Ship Immediately
Specifications
Series: --
Packaging: Tape & Reel (TR) 
Part Status: Not For New Designs
Transistor Type: PNP
Current - Collector (Ic) (Max): 1A
Voltage - Collector Emitter Breakdown (Max): 80V
Vce Saturation (Max) @ Ib, Ic: 400mV @ 50mA, 500mA
Current - Collector Cutoff (Max): 1µA (ICBO)
DC Current Gain (hFE) (Min) @ Ic, Vce: 120 @ 100mA, 3V
Power - Max: 10W
Frequency - Transition: 100MHz
Operating Temperature: 150°C (TJ)
Mounting Type: Surface Mount
Package / Case: TO-252-3, DPak (2 Leads + Tab), SC-63
Supplier Device Package: CPT3
Base Part Number: 2SB1181
Description

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The 2SB1181TLR is a high-voltage, dual NPN complementary epitaxial silicon transistor. It is the most common type of single bipolar junction transistor (BJT) commonly used in many applications. The 2SB1181TLR is a low-power device that is intended for use as an amplifier, switch, and an analog signal processor. This article will provide an overview of the 2SB1181TLR\'s application field, and its working principle.

Applications of the 2SB1181TLR

The 2SB1181TLR is well-suited for use in low-power amplifier circuits, and it is also often used in switch and signal circuits. Its applications include but are not limited to:

  • Audio amplifiers
  • Transistor switches
  • Audio power amplifiers
  • Logic circuits
  • Power supplies
  • Analog signal processor
  • Radio frequency (RF) amplifiers
  • Motor control circuits

The 2SB1181TLR is often used as a low-power, class A amplifier as it was designed for use in audio circuits. This device is also well-suited for use in switch and signal circuits, as well as in circuits requiring fast switching speed, such as radio-frequency amplifiers. Additionally, due to its low collector-emitter saturation voltage, the 2SB1181TLR is well-suited for use in circuits where voltage regulation is required.

Working Principle of the 2SB1181TLR

The 2SB1181TLR is a single NPN-complementary BJT. It is composed of two p-type semiconductor materials and two n-type semiconductor materials which form the transistor\'s base, collector and emitter. The 2SB1181TLR has a current gain between 30 to 100, depending on the collector current for operation. The device operates in a saturated state when the voltage between the base and the emitter is greater than the cut-in voltage of the device. This state is referred to as the Linear Region, and it results in a constant current gain for the device.

In order for the 2SB1181TLR to operate, the base is first supplied with a voltage from a source. This voltage attracts electrons from the base to the collector and provides a path for the current to flow from the emitter to the collector. The current gain of the device is determined by the ratio of the voltage between the base and emitter to the voltage between the collector and emitter. As the base-emitter voltage increases, more current is allowed to flow and the transistor enters the saturated state.

Once the device is in the saturated state, the current gain is no longer constant and is then determined by the current flowing through the transistor. The collector current will continue to increase until the base-emitter voltage reaches the maximum collector-emitter saturation voltage, or Vce(sat). At this point, the transistor cannot allow any more current to flow from the collector to the emitter and the device is said to be in the Cut-Off State.

Conclusion

The 2SB1181TLR is a high-voltage, low-power dual NPN complementary epitaxial silicon transistor. It is used in many applications such as audio amplifiers, transistor switches, as an analog signal processor and in motor control circuits. Its working principle involves the flow of current from the base to the collector and then to the emitter to amplify the signal. The current gain of the device is determined by the ratio of the voltage between the base and emitter to the voltage between the collector and emitter. It is an ideal choice for low-power applications, and its ability to operate in saturated and cut-off states makes it suitable for a variety of uses.

The specific data is subject to PDF, and the above content is for reference

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