Allicdata Part #: | 2N7053_D26Z-ND |
Manufacturer Part#: |
2N7053_D26Z |
Price: | $ 0.00 |
Product Category: | Discrete Semiconductor Products |
Manufacturer: | ON Semiconductor |
Short Description: | TRANS NPN DARL 100V 1.5A TO-226 |
More Detail: | Bipolar (BJT) Transistor NPN - Darlington 100V 1.5... |
DataSheet: | 2N7053_D26Z Datasheet/PDF |
Quantity: | 1000 |
1 +: | 0.00000 |
Series: | -- |
Packaging: | Tape & Reel (TR) |
Part Status: | Obsolete |
Transistor Type: | NPN - Darlington |
Current - Collector (Ic) (Max): | 1.5A |
Voltage - Collector Emitter Breakdown (Max): | 100V |
Vce Saturation (Max) @ Ib, Ic: | 1.5V @ 100µA, 100mA |
Current - Collector Cutoff (Max): | 200nA |
DC Current Gain (hFE) (Min) @ Ic, Vce: | 1000 @ 1A, 5V |
Power - Max: | 1W |
Frequency - Transition: | 200MHz |
Operating Temperature: | -55°C ~ 150°C (TJ) |
Mounting Type: | Through Hole |
Package / Case: | TO-226-3, TO-92-3 Long Body (Formed Leads) |
Supplier Device Package: | TO-226 |
Base Part Number: | 2N7053 |
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2N7053_D26Z Application Field and Working Principle
The 2N7053_D26Z is a single bipolar junction transistor (BJT), which is made up of an emitter, a base, and a collector. The emitter is the source of the electrons and the collector is the target of the electrons. The base serves as the reverse biased region, preventing current flow between the emitter and the collector. When an external electric field is applied to the BJT, the electrons are able to cross the reverse biased region and flow from the emitter to the collector. Thus, the BJT allows efficient current control.
Application Fields
BJTs are widely used across many application fields. In power applications, BJTs can be used to control large amounts of current in power management systems for motor drivers and other power circuits. Moreover, BJTs can be used in digital logic circuits such as logic gates, amplifiers, and comparators. Lastly, BJTs are used in analog applications such as audio amplifiers, radio frequency amplifiers, and oscillators.
Structure and Working Principle
BJTs consist of five regions: emitter, base, collector, emitter junction, and collector junction. The emitter junction is the area between the emitter and the base, and the collector junction is the area between the collector and the base. The emitter and collector of the BJT are two different regions separated by a thin and heavily doped semiconductor layer. This semiconductor layer, called the base, is where the current flow is controlled. The application of an external electric field to the BJT deformates and forces some electrons from the emitter to the collector.
In order for current to flow through the BJT, the base-emitter voltage must be greater than the base-collector voltage. The application of this external electric field will increase the electrical potential threshold from the base to the emitter, and the electrons from the emitter will start to flow towards the collector. The current flow is controlled by the transistor\'s current gain and voltage gain. The transistor\'s current gain is the ratio of the collector-emitter current to the base-emitter current, while the voltage gain is the ratio of the collector-emitter voltage to the base-collector voltage.
When the base-emitter voltage is greater than the base-collector voltage, a larger electric field allows more electrons to flow from the emitter to the collector. Hence, BJTs can be used to control and regulate current flow in circuits. The current gain of a BJT is determined by the ratio of electrons injected from the emitter to the collector, which is denoted by the parameter hFE. The higher the hFE, the higher the current gain.
Conclusion
In conclusion, the 2N7053_D26Z is a single bipolar junction transistor (BJT), which is made up of an emitter, a base, and a collector. The application of an external electric field to the BJT allows electrons to flow from the emitter to the collector, allowing efficient current control. BJTs are widely used across many application fields such as power applications, digital logic circuits, and analog applications. The current flow is controlled by the transistor\'s current gain and voltage gain. The current gain of a BJT is determined by the ratio of electrons injected from the emitter to the collector, which is denoted by the parameter hFE.
The specific data is subject to PDF, and the above content is for reference
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