Allicdata Part #: | MS1801-ND |
Manufacturer Part#: |
MS1801 |
Price: | $ 0.00 |
Product Category: | Discrete Semiconductor Products |
Manufacturer: | Microsemi Corporation |
Short Description: | RF POWER TRANSISTOR |
More Detail: | RF Transistor |
DataSheet: | MS1801 Datasheet/PDF |
Quantity: | 1000 |
1 +: | 0.00000 |
Series: | -- |
Part Status: | Obsolete |
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The MS1801 application field and working principle is a type of transistor based on the bipolar junction transistor (BJT). This transistor is widely used in radio frequency (RF) applications, such as in radio transmitter and receiver, or in the design of power amplifiers and oscillators. The MS1801 is a powerful, cost-effective transistor that is used in various applications.
A bipolar junction transistor (BJT) is a three-terminal device, usually consisting of three semiconductor layers, each of which has a slightly different energy band gap, allowing current carriers to move in specific directions. The semiconductor layers of the BJT are usually the emitter, base, and collector with typically 10 to 100 times the base-emitter voltage applied to the base–emitter junction. The BJT transistor operating in the forward and reverse bias modes act as both a switch and an amplifier.
The MS1801 transistor is an NPN bipolar junction transistor, which means that the base is N-type semiconductor, the emitter is P-type, and the collector is N-type. The MS1801 is specifically designed for use in high-power radio frequency (RF) applications. It has a low noise level and good gain linearity. It also has good reverse recovery time and excellent ESD protection.
To understand the operation of the MS1801, it helps to consider its terminals as analogous to "gates" or "paths" through which electrons can move. When a voltage is applied across the base-emitter junction, it creates an electric field, which causes electrons to be attracted from the base to the emitter. This leads to current flow from the base to the emitter. Then, a rising voltage on the collector allows electrons from the emitter to flow into the collector, commonly referred to as "collector current" which is proportional to the voltage applied to the base-emitter junction.
The maximum collector-emitter voltage (Vce) of the MS1801 is 30 Volts, and its Voltage gain is about 25. The current gain, or β of the transistor is typically 80 to 120. The high-frequency cutoffs (fT) of the transistor are typically 1.3GHz and its maximum frequency of oscillation (ft) is usuallyaround 500MHz. The MS1801 is typically used in applications such as radio receivers, television tuners and digital circuitry, with applications including amplifiers, transmitters, oscillators, and signal processing.
In operation, the MS1801 transistor can be used to amplify, provide gain, and provide impedance matching in a variety of applications. Its features make it useful in applications in which very low noise, high gain and excellent linearity are desired. The MS1801 transistor is used to provide gain in RF amplifiers and oscillators, in which very low noise is desired. It is also used to provide input and output impedance matching, as well as to convert a logic level signal to a higher power signal.
The MS1801is also used in a variety of audio applications, such as audio switching, detection and amplification. The low noise feature of the MS1801 allows for a wide range of audio applications.It can be used in filters to reduce noise, and as an active component in audio amplifiers. It can also be used in applications where a high amount of voltage gain is required.
The MS1801 is a common transistor used in many applications. Its features, such as low noise, excellent linearity and high-power capabilities, make it an ideal choice for RF applications. It can be used to provide gain, impedance matching and audio switching, making it a versatile device for many applications.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
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MS1801 | Microsemi Co... | 0.0 $ | 1000 | RF POWER TRANSISTORRF Tra... |
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MS18130-10RU | Vishay Dale | 0.0 $ | 1000 | IM-4 1.5 10% MS18130-10 R... |
MS18130-10SH | Vishay Dale | 0.0 $ | 1000 | IM-4 1.5 10% MS18130-10 R... |
MS18130-10ST | Vishay Dale | 0.0 $ | 1000 | IM-4 1.5 10% MS18130-10 R... |
MS18130-11BH | Vishay Dale | 0.0 $ | 1000 | IM-4 1.8 10% MS18130-11 B... |
MS18130-11RU | Vishay Dale | 0.0 $ | 1000 | IM-4 1.8 10% MS18130-11 R... |
MS18130-11SH | Vishay Dale | 0.0 $ | 1000 | IM-4 1.8 10% MS18130-11 R... |
MS18130-11ST | Vishay Dale | 0.0 $ | 1000 | IM-4 1.8 10% MS18130-11 R... |
MS18130-12BH | Vishay Dale | 0.0 $ | 1000 | IM-4 2.2 10% MS18130-12 B... |
MS18130-12RU | Vishay Dale | 0.0 $ | 1000 | IM-4 2.2 10% MS18130-12 R... |
MS18130-12SH | Vishay Dale | 0.0 $ | 1000 | IM-4 2.2 10% MS18130-12 R... |
MS18130-12ST | Vishay Dale | 0.0 $ | 1000 | IM-4 2.2 10% MS18130-12 R... |
MS18130-13BH | Vishay Dale | 0.0 $ | 1000 | IM-4 2.7 10% MS18130-13 B... |
MS18130-13RU | Vishay Dale | 0.0 $ | 1000 | IM-4 2.7 10% MS18130-13 R... |
MS18130-14BH | Vishay Dale | 0.0 $ | 1000 | IM-4 3.3 10% MS18130-14 B... |
MS18130-14RU | Vishay Dale | 0.0 $ | 1000 | IM-4 3.3 10% MS18130-14 R... |
MS18130-14SH | Vishay Dale | 0.0 $ | 1000 | IM-4 3.3 10% MS18130-14 R... |
MS18130-14ST | Vishay Dale | 0.0 $ | 1000 | IM-4 3.3 10% MS18130-14 R... |
MS18130-15BH | Vishay Dale | 0.0 $ | 1000 | IM-4 3.9 10% MS18130-15 B... |
MS18130-15RU | Vishay Dale | 0.0 $ | 1000 | IM-4 3.9 10% MS18130-15 R... |
MS18130-15SH | Vishay Dale | 0.0 $ | 1000 | IM-4 3.9 10% MS18130-15 R... |
MS18130-16ST | Vishay Dale | 0.0 $ | 1000 | IM-4 4.7 10% MS18130-16 R... |
MS18130-1RU | Vishay Dale | 0.0 $ | 1000 | IM-4 .15 20% MS18130-1 R3... |
MS18130-1ST | Vishay Dale | 0.0 $ | 1000 | IM-4 .15 20% MS18130-1 RJ... |
MS18130-2BH | Vishay Dale | 0.0 $ | 1000 | IM-4 .22 20% MS18130-2 B0... |
MS18130-2SH | Vishay Dale | 0.0 $ | 1000 | IM-4 .22 20% MS18130-2 RJ... |
MS18130-2ST | Vishay Dale | 0.0 $ | 1000 | IM-4 .22 20% MS18130-2 RJ... |
MS18130-3BH | Vishay Dale | 0.0 $ | 1000 | IM-4 .33 20% MS18130-3 B0... |
MS18130-3RU | Vishay Dale | 0.0 $ | 1000 | IM-4 .33 20% MS18130-3 R3... |
MS18130-3SH | Vishay Dale | 0.0 $ | 1000 | IM-4 .33 20% MS18130-3 RJ... |
MS18130-3ST | Vishay Dale | 0.0 $ | 1000 | IM-4 .33 20% MS18130-3 RJ... |
MS18130-4BH | Vishay Dale | 0.0 $ | 1000 | IM-4 .47 20% MS18130-4 B0... |
MS18130-4RU | Vishay Dale | 0.0 $ | 1000 | IM-4 .47 20% MS18130-4 R3... |
MS18130-4SH | Vishay Dale | 0.0 $ | 1000 | IM-4 .47 20% MS18130-4 RJ... |
MS18130-4ST | Vishay Dale | 0.0 $ | 1000 | IM-4 .47 20% MS18130-4 RJ... |
MS18130-5BH | Vishay Dale | 0.0 $ | 1000 | IM-4 .56 10% MS18130-5 B0... |
MS18130-15ST | Vishay Dale | 0.0 $ | 1000 | IM-4 3.9 10% MS18130-15 R... |
MS18130-16BH | Vishay Dale | 0.0 $ | 1000 | IM-4 4.7 10% MS18130-16 B... |
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