Allicdata Part #: | CW0102K000JB12-ND |
Manufacturer Part#: |
CW0102K000JB12 |
Price: | $ 0.85 |
Product Category: | Resistors |
Manufacturer: | Vishay Dale |
Short Description: | RES 2K OHM 13W 5% AXIAL |
More Detail: | 2 kOhms ±5% 13W Through Hole Resistor Axial Moistu... |
DataSheet: | CW0102K000JB12 Datasheet/PDF |
Quantity: | 1000 |
100 +: | $ 0.77396 |
300 +: | $ 0.66339 |
500 +: | $ 0.55283 |
1000 +: | $ 0.47912 |
5000 +: | $ 0.46437 |
Series: | CW |
Packaging: | Bulk |
Part Status: | Active |
Resistance: | 2 kOhms |
Tolerance: | ±5% |
Power (Watts): | 13W |
Composition: | Wirewound |
Features: | Moisture Resistant |
Temperature Coefficient: | ±30ppm/°C |
Operating Temperature: | -65°C ~ 350°C |
Package / Case: | Axial |
Supplier Device Package: | Axial |
Size / Dimension: | 0.375" Dia x 1.781" L (9.52mm x 45.24mm) |
Height - Seated (Max): | -- |
Number of Terminations: | 2 |
Failure Rate: | -- |
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Through Hole Resistors have been around in various forms since the beginning of the electrical engineering world. The symbol most associated with these components is the cylindrical shell with evenly spaced pins out each end. One of these popular types, the CW0102K000JB12, are often referred to as through-hole resistors and are used to control electrical current in circuits.
In general, through-hole resistors are made of closely wound material with insulated ends. The material is typically ceramic or metal. The two separate pins at each end provide connections to make the electrical current flow through the resistor. Generally speaking, they are used to control current, provide impedance, divide voltages and protect circuits.
The CW0102K000JB12 is a small cylinder-shaped through-hole resistor with two pins that protrude from two opposite sides of the shell. The resistor is closely wound with insulated copper wire and can handle temperatures up to 350 degrees Celsius. The CW0102K000JB12 is especially used in high-temperature environments such as aircraft and spacecraft applications. It is also used in RF/microwave applications, and in some other medical and industrial applications.
The working principle of the CW0102K000JB12 is simple in concept. By connecting one of the pins to a negative supply voltage and the other pin to a positive supply voltage, an electrical signal is sent through the resistor. This signal will be reduced by the resistor. The amount of energy that is lost depends on the ohmic value of the resistor. The ohmic value is the amount of energy that is lost when a current passes through the resistor. This ohmic value is usually expressed as a number, typically ranging from 1 to 10 ohms.
The CW0102K000JB12 is often used when high-temperature stability is needed. It is also used when a higher level of precision is desired and when a more reliable resistor is desired. It is important to note that the CW0102K000JB12 will not work alone in an application; it must be used in conjunction with other components in order to provide the desired level of resistance.
Overall, the CW0102K000JB12 is a popular choice for various applications that demand precision and thermal stability. It is a reliable resistor that can be used in a variety of applications, from high-temperature environments and RF/microwave applications to medical and industrial applications. Through its simple working principle and accurate ohmic value, it can easily provide the desired level of resistance and electrical current control for a given application.
The specific data is subject to PDF, and the above content is for reference
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CW010120K0JE73HS | Vishay Dale | 0.8 $ | 1000 | RES 120K OHM 13W 5% AXIAL... |
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CW010150K0JE73HS | Vishay Dale | 0.8 $ | 1000 | RES 150K OHM 13W 5% AXIAL... |
CW010160K0JE73HS | Vishay Dale | 0.8 $ | 1000 | RES 160K OHM 13W 5% AXIAL... |
CW010499R0JE12HE | Vishay Dale | 0.8 $ | 1000 | RES 499 OHM 13W 5% AXIAL4... |
CW01010K00JB12 | Vishay Dale | 0.85 $ | 1000 | RES 10K OHM 13W 5% AXIAL1... |
CW0101K200JB12 | Vishay Dale | 0.85 $ | 1000 | RES 1.2K OHM 13W 5% AXIAL... |
CW0101K200JB123 | Vishay Dale | 0.85 $ | 1000 | RES 1.2K OHM 13W 5% AXIAL... |
CW0101K250JB12 | Vishay Dale | 0.85 $ | 1000 | RES 1.25K OHM 13W 5% AXIA... |
CW0101K500JB12 | Vishay Dale | 0.85 $ | 1000 | RES 1.5K OHM 13W 5% AXIAL... |
CW0101K600JB12 | Vishay Dale | 0.85 $ | 1000 | RES 1.6K OHM 13W 5% AXIAL... |
CW0101K750JB12 | Vishay Dale | 0.85 $ | 1000 | RES 1.75K OHM 13W 5% AXIA... |
CW0101K800JB12 | Vishay Dale | 0.85 $ | 1000 | RES 1.8K OHM 13W 5% AXIAL... |
CW0101K900JB12 | Vishay Dale | 0.85 $ | 1000 | RES 1.9K OHM 13W 5% AXIAL... |
CW0102K000JB12 | Vishay Dale | 0.85 $ | 1000 | RES 2K OHM 13W 5% AXIAL2 ... |
CW0102K000JB123 | Vishay Dale | 0.85 $ | 1000 | RES 2K OHM 13W 5% AXIAL2 ... |
CW0102K200JB12 | Vishay Dale | 0.85 $ | 1000 | RES 2.2K OHM 13W 5% AXIAL... |
CW0102K250JB12 | Vishay Dale | 0.85 $ | 1000 | RES 2.25K OHM 13W 5% AXIA... |
CW0102K500JB12 | Vishay Dale | 0.85 $ | 1000 | RES 2.5K OHM 13W 5% AXIAL... |
CW0102K500JB123 | Vishay Dale | 0.85 $ | 1000 | RES 2.5K OHM 13W 5% AXIAL... |
CW0102K700JB12 | Vishay Dale | 0.85 $ | 1000 | RES 2.7K OHM 13W 5% AXIAL... |
CW0103K000JB12 | Vishay Dale | 0.85 $ | 1000 | RES 3K OHM 13W 5% AXIAL3 ... |
CW0103K100JB12 | Vishay Dale | 0.85 $ | 1000 | RES 3.1K OHM 13W 5% AXIAL... |
CW0103K300JB12 | Vishay Dale | 0.85 $ | 1000 | RES 3.3K OHM 13W 5% AXIAL... |
CW0103K500JB12 | Vishay Dale | 0.85 $ | 1000 | RES 3.5K OHM 13W 5% AXIAL... |
CW0103K600JB12 | Vishay Dale | 0.85 $ | 1000 | RES 3.6K OHM 13W 5% AXIAL... |
CW0103K900JB12 | Vishay Dale | 0.85 $ | 1000 | RES 3.9K OHM 13W 5% AXIAL... |
CW0104K000JB12 | Vishay Dale | 0.85 $ | 1000 | RES 4K OHM 13W 5% AXIAL4 ... |
CW0104K700JB12 | Vishay Dale | 0.85 $ | 1000 | RES 4.7K OHM 13W 5% AXIAL... |
CW0105K000JB12 | Vishay Dale | 0.85 $ | 1000 | RES 5K OHM 13W 5% AXIAL5 ... |
CW0105K000JB123 | Vishay Dale | 0.85 $ | 1000 | RES 5K OHM 13W 5% AXIAL5 ... |
CW0105K100JB12 | Vishay Dale | 0.85 $ | 1000 | RES 5.1K OHM 13W 5% AXIAL... |
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