Allicdata Part #: | FCR50SJT-52-1K2-ND |
Manufacturer Part#: |
FCR50SJT-52-1K2 |
Price: | $ 0.01 |
Product Category: | Resistors |
Manufacturer: | Yageo |
Short Description: | RES 1/2W 5% AXIAL |
More Detail: | 1.2 kOhms ±5% 0.5W, 1/2W Through Hole Resistor Axi... |
DataSheet: | FCR50SJT-52-1K2 Datasheet/PDF |
Quantity: | 1000 |
5000 +: | $ 0.00482 |
Series: | FCR |
Packaging: | Tape & Box (TB) |
Part Status: | Active |
Resistance: | 1.2 kOhms |
Tolerance: | ±5% |
Power (Watts): | 0.5W, 1/2W |
Composition: | Carbon Film |
Features: | Flame Proof, Safety |
Temperature Coefficient: | -500/ +350ppm/°C |
Operating Temperature: | -55°C ~ 155°C |
Package / Case: | Axial |
Supplier Device Package: | Axial |
Size / Dimension: | 0.094" Dia x 0.248" L (2.40mm x 6.30mm) |
Height - Seated (Max): | -- |
Number of Terminations: | 2 |
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Through Hole Resistors, such as FCR50SJT-52-1K2, are essential components in electrical engineering, as they are used in a variety of applications. Throughout a variety of applications, through hole resistors are often used to control the amount of voltage or current in a circuit. These components have different types and characteristics. To understand the application field and working principle of the FCR50SJT-52-1K2, it is important to know the basic principles of electrical engineering and understand how the resistor works.
A through hole resistor is a passive element that can be used to restrict the flow of electricity in an electrical circuit. It works mainly by creating a certain amount of resistance that reduces the amount of current flowing through a circuit. Depending on the level of resistance, these components can be rated as high or low resistance. In particular, FCR50SJT-52-1K2 is a low resistance through hole resistor with a wide operating temperature range (-55 to +125 C).
The FCR50SJT-52-1K2 consists of a ceramic body and copper alloy terminal, enabling it to withstand a high amount of thermal energy. The ceramic body is filled with a resistor element or oxide to provide a precise resistance. The rated value of a resistor depends on the material of the resistor element, the length of the resistor and the cross section of the resistor. In the FCR50SJT-52-1K2, the resistor element is made of manganese-nickel (Mn/Ni) alloy and is 0.03" x 0.125" in size. This ensures a nominal resistance value of 1K2 (1.2K ohm).
The application field of a through hole resistor is mainly related to the rated value and the power dissipation. The FCR50SJT-52-1K2 has a wide application field in electronics, as it can be used for different applications with its low resistance values and high power dissipation. It can be used in other applications such as bypass circuits, voltage dividers, waveform shaping and temperature compensation. Its wide operating temperature range also makes it suitable for cryogenic applications and temperature measurement.
In addition, FCR50SJT-52-1K2 has a wide power dissipation range, enabling it to use in applications with high-current draws. This is because the power dissipation of a resistor is directly related to the amount of heat produced. The higher the power dissipation, the more heat it can dissipate without being damaged. This makes it perfect for high current applications, such as inductive circuits, which draw a lot of current.
The working principle of a through hole resistor is simple. When an electrical current flows through a resistor, the resistor changes the amount of current that flows through the circuit. This is due to its ability to convert electrical energy into heat energy. This principle can be used in various applications in electronics, including voltage and current control, protection, and waveform shaping. The FCR50SJT-52-1K2 is an ideal component for these applications due to its wide operating temperature range and high power dissipation.
In conclusion, the FCR50SJT-52-1K2 is a low resistance through hole resistor with a wide operating temperature range and high power dissipation. It is a versatile component that can be used in various applications, including bypass circuits, voltage dividers, waveform shaping, and temperature compensation. Its working principle is based on its ability to convert electrical energy into heat energy, which allows it to control the amount of current and voltage flowing through a circuit.
The specific data is subject to PDF, and the above content is for reference
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FCR50SJT-52-200K | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL200 kOhm... |
FCR50SJT-52-100K | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL100 kOhm... |
FCR50SJT-52-100R | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL100 Ohms... |
FCR50SJT-52-10K | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL10 kOhms... |
FCR50SJT-52-10R | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL10 Ohms ... |
FCR50SJT-52-110K | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL110 kOhm... |
FCR50SJT-52-110R | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL110 Ohms... |
FCR50SJT-52-11K | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL11 kOhms... |
FCR50SJT-52-11R | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL11 Ohms ... |
FCR50SJT-52-120K | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL120 kOhm... |
FCR50SJT-52-120R | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL120 Ohms... |
FCR50SJT-52-12K | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL12 kOhms... |
FCR50SJT-52-12R | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL12 Ohms ... |
FCR50SJT-52-130K | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL130 kOhm... |
FCR50SJT-52-130R | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL130 Ohms... |
FCR50SJT-52-13K | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL13 kOhms... |
FCR50SJT-52-13R | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL13 Ohms ... |
FCR50SJT-52-150K | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL150 kOhm... |
FCR50SJT-52-150R | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL150 Ohms... |
FCR50SJT-52-15K | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL15 kOhms... |
FCR50SJT-52-15R | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL15 Ohms ... |
FCR50SJT-52-160K | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL160 kOhm... |
FCR50SJT-52-160R | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL160 Ohms... |
FCR50SJT-52-16K | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL16 kOhms... |
FCR50SJT-52-16R | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL16 Ohms ... |
FCR50SJT-52-180K | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL180 kOhm... |
FCR50SJT-52-180R | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL180 Ohms... |
FCR50SJT-52-18K | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL18 kOhms... |
FCR50SJT-52-18R | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL18 Ohms ... |
FCR50SJT-52-1K | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL1 kOhms ... |
FCR50SJT-52-1K1 | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL1.1 kOhm... |
FCR50SJT-52-1K2 | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL1.2 kOhm... |
FCR50SJT-52-1K3 | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL1.3 kOhm... |
FCR50SJT-52-1K5 | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL1.5 kOhm... |
FCR50SJT-52-1K6 | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL1.6 kOhm... |
FCR50SJT-52-1K8 | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL1.8 kOhm... |
FCR50SJT-52-1M | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL1 MOhms ... |
FCR50SJT-52-200R | Yageo | 0.01 $ | 1000 | RES 1/2W 5% AXIAL200 Ohms... |
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