Allicdata Part #: | 541-2769-ND |
Manufacturer Part#: |
CW01027R00JE12HE |
Price: | $ 1.39 |
Product Category: | Resistors |
Manufacturer: | Vishay Dale |
Short Description: | RES 27 OHM 13W 5% AXIAL |
More Detail: | 27 Ohms ±5% 13W Through Hole Resistor Axial Wirew... |
DataSheet: | CW01027R00JE12HE Datasheet/PDF |
Quantity: | 76 |
1 +: | $ 1.26000 |
10 +: | $ 1.12500 |
25 +: | $ 1.05750 |
50 +: | $ 0.96750 |
Series: | CW |
Packaging: | Bulk |
Part Status: | Active |
Resistance: | 27 Ohms |
Tolerance: | ±5% |
Power (Watts): | 13W |
Composition: | Wirewound |
Features: | -- |
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 are a type of passive component found in a variety of electronic circuits. They are typically used to adjust the voltage and current levels in circuits and are identified by their physical properties such as the size, shape and material composition of their bodies. The CW01027R00JE12HE model is a through hole resistor specifically designed for the power industry.
This particular model is a type of metal-oxide-semiconductor field-effect transistor (MOSFET) which is a three terminal device that features a metal oxide gate. The metal oxide gate is composed of a metal gate over a thin layer of oxide, allowing a variable electric field to be applied across the terminal. This means that the resistor is capable of controlling large voltages or currents and thus is used in many power-related applications such as power transformers, AC/DC switching supplies and solar panels.
The working principle behind this model is such that when the metal-oxide-semiconductor is exposed to an electric field the resistance of the resistor will change. This process allows the resistor to adjust the current and voltage levels in a circuit. The advantages of this resistor include high power transfer and high switching speeds which make it highly suitable for fast switching and power transfer applications.
In conclusion, the CW01027R00JE12HE is a type of through hole resistor specifically designed for the power industry. It features a metal oxide gate allowing a variable electric field to be applied across its terminals. The working principle behind this resistor is such that when exposed to an electric field the resistance of the resistor will change, allowing it to adjust current and voltage levels in a circuit. Its advantages include high power transfer and high switching speeds making it suitable for fast switching and power transfer applications.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
CW01050R00HE12 | Vishay Dale | 0.79 $ | 1000 | RES 50 OHM 13W 3% AXIAL50... |
CW0105R000HE12 | Vishay Dale | 0.79 $ | 1000 | RES 5 OHM 13W 3% AXIAL5 O... |
CW0107R500HE12 | Vishay Dale | 0.79 $ | 1000 | RES 7.5 OHM 13W 3% AXIAL7... |
CW010130K0JE733 | Vishay Dale | 0.8 $ | 1000 | RES 130K OHM 13W 5% AXIAL... |
CW010130K0KE733 | Vishay Dale | 0.8 $ | 1000 | RES 130K OHM 13W 10% AXIA... |
CW010150K0JE733 | Vishay Dale | 0.8 $ | 1000 | RES 150K OHM 13W 5% AXIAL... |
CW010150K0KE733 | Vishay Dale | 0.8 $ | 1000 | RES 150K OHM 13W 10% AXIA... |
CW010110K0JE73HS | Vishay Dale | 0.8 $ | 1000 | RES 110K OHM 13W 5% AXIAL... |
CW010120K0JE73HS | Vishay Dale | 0.8 $ | 1000 | RES 120K OHM 13W 5% AXIAL... |
CW010130K0JE73HS | Vishay Dale | 0.8 $ | 1000 | RES 130K OHM 13W 5% AXIAL... |
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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