Allicdata Part #: | ZTX603STZ-ND |
Manufacturer Part#: |
ZTX603STZ |
Price: | $ 0.29 |
Product Category: | Discrete Semiconductor Products |
Manufacturer: | Diodes Incorporated |
Short Description: | TRANS NPN DARL 80V 1A E-LINE |
More Detail: | Bipolar (BJT) Transistor NPN - Darlington 80V 1A 1... |
DataSheet: | ZTX603STZ Datasheet/PDF |
Quantity: | 1000 |
2000 +: | $ 0.25516 |
Series: | -- |
Packaging: | Tape & Box (TB) |
Part Status: | Active |
Transistor Type: | NPN - Darlington |
Current - Collector (Ic) (Max): | 1A |
Voltage - Collector Emitter Breakdown (Max): | 80V |
Vce Saturation (Max) @ Ib, Ic: | 1V @ 1mA, 1A |
Current - Collector Cutoff (Max): | 10µA |
DC Current Gain (hFE) (Min) @ Ic, Vce: | 2000 @ 1A, 5V |
Power - Max: | 1W |
Frequency - Transition: | 150MHz |
Operating Temperature: | -55°C ~ 200°C (TJ) |
Mounting Type: | Through Hole |
Package / Case: | E-Line-3, Formed Leads |
Supplier Device Package: | E-Line (TO-92 compatible) |
Base Part Number: | ZTX603 |
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The ZTX603STZ is a single-transistor bipole type transistor designed for linear small signal amplifiers such as low-frequency amplifiers, oscillator stages, high-frequency amplifiers, and active filters. This type of transistor is a widely used component for these applications due to its excellent operating characteristics and performance. This article will discuss the application field and working principles of the ZTX603STZ.
The ZTX603STZ is a bipolar NPN transistor that has a numeric equivalent of the BC327. Its maximum collector current is -600mA and its maximum voltage gain is 1100. It is equipped with an emitter-base breakdown voltage of 4.5V, a collector-base breakdown voltage of 15V, and a maximum power dissipation of 625mW. Furthermore, the ZTX603STZ has an operating temperature range of -65°C to +100°C and a storage temperature range of -65°C to +150°C, making it a very suitable component for operation in a wide range of temperatures.
The ZTX603STZ can be used for linear small signal amplifiers, making it suitable for low-frequency amplifiers, oscillator stages, high-frequency amplifiers, and active filters. As a bipolar transistor, it works by relying on the flow of electrons and holes within the component, which are then collected and emitted from the P-type (holes) and N-type (electrons) regions of the component. In this way, the current gain of the component, also known as the current amplification coefficient or β, is determined by the ratio of the doping concentrations in the different regions of the component.
The ZTX603STZ can be used in an amplifier configuration, where it will be used to amplify the input signal. The transistor will function as the input, amplification, and output stages of an amplifier by allowing the input signal to control the current flow between the base and collector regions. This, in turn, will result in a larger output signal from the collector region that is of the same shape and frequency as the input signal. When the output signal is larger than the input signal, the amplifier is said to have been successfully amplified the signal, creating an output with gain.
The ZTX603STZ is also used in oscillator and active filter designs. In oscillator designs, the transistor will be used in an amplifier configuration that is connected to a feedback loop, allowing the input signal to oscillate at a stable frequency and create the required oscillation. In active filter designs, the amplifier and transistor combination will be used to create sophisticated filtering that can isolate and amplify specific frequency ranges. The transistor will be connected in a specific configuration, such as an RC network, that will allow it to filter out the desired frequencies and create a output signal with the required characteristics.
In conclusion, the ZTX603STZ is a single-transistor bipole type transistor designed for linear small signal amplifiers. Its excellent characteristics and performance make it suitable for use in low-frequency amplifiers, oscillator stages, high-frequency amplifiers, and active filters. It depends on the flow of electrons and holes within the component to determine the current gain of the component and can be used in amplifier, oscillator, and active filter configurations to create the desired output signal.
The specific data is subject to PDF, and the above content is for reference
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