| Allicdata Part #: | 1263-CF14JB390K-CHP |
| Manufacturer Part#: |
CF14JB390K |
| Price: | $ 0.01 |
| Product Category: | Resistors |
| Manufacturer: | Stackpole Electronics Inc. |
| Short Description: | RES 390K OHM 1/4W 5% AXIAL |
| More Detail: | 390 kOhms ±5% 0.25W, 1/4W Through Hole Resistor Ax... |
| DataSheet: | CF14JB390K Datasheet/PDF |
| Quantity: | 14000 |
| 1000 +: | $ 0.00505 |
| 2000 +: | $ 0.00436 |
| 5000 +: | $ 0.00390 |
| 10000 +: | $ 0.00350 |
| Series: | CF |
| Packaging: | Bulk |
| Part Status: | Active |
| Resistance: | 390 kOhms |
| Tolerance: | ±5% |
| Power (Watts): | 0.25W, 1/4W |
| Composition: | Carbon Film |
| Features: | Flame Retardant Coating, Safety |
| Temperature Coefficient: | 0/ -850ppm/°C |
| Operating Temperature: | -55°C ~ 155°C |
| Package / Case: | Axial |
| Supplier Device Package: | Axial |
| Size / Dimension: | 0.091" Dia x 0.236" L (2.30mm x 6.00mm) |
| Height - Seated (Max): | -- |
| Number of Terminations: | 2 |
| Failure Rate: | -- |
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Through Hole Resistors are electronic components designed to control the flow of electricity in circuits. CF14JB390K is one of these Through Hole Resistor components, and it is used for a variety of applications. In this article, we will discuss the application field and working principle of a CF14JB390K Through Hole Resistor.
A CF14JB390K Through Hole Resistor is designed for applications that involve higher voltages and currents. This makes it suitable for a wide range of uses, such as electric motors, servo drives, power supplies, inverters, and so on. The CF14JB390K Through Hole Resistor also has excellent power dissipation ratings, making it ideal for use in high-power circuits.
The construction of a CF14JB390K Through Hole Resistor is quite simple. It consists of a body or “rail” made up of dielectric material, typically ceramic or plastic. The dielectric is then filled with metal coating, usually aluminum, which acts as an insulative material. This metal coating is in turn covered by a layer of metalized glass, which provides the basic resistance value of the resistor.
The working principle of a CF14JB390K Through Hole Resistor is relatively simple. When electricity is sent through the resistor, a small amount of electricity is lost to the resistance of the component, thus reducing the voltage and current being sent through the circuit. This is achieved by the metalized glass layer, which acts as an insulator, preventing the flow of electricity through the resistor and causing the loss of voltage and current.
The resistance value of a CF14JB390K Through Hole Resistor can be adjusted in a number of ways. The number of layers of metalized glass layered on top of the dielectric material will affect the resistance value. Different types of dielectric materials may also be used. The resistance value can be further increased or decreased by changing the amount of aluminum in the metalized glass layer.
In conclusion, a CF14JB390K Through Hole Resistor is a very versatile component, suitable for a wide range of applications. It is constructed of a body or “rail” made of dielectric material, usually ceramic or plastic, filled with metal coating, usually aluminum, and covered by a layer of metalized glass. The working principle is simply that electricity is sent through the resistor, a small portion of which is lost to the resistance of the component, thus reducing the voltage and current sent through the circuit. The resistance value can be adjusted in a number of ways by changing the number of layers of metalized glass, using different types of dielectric materials, or by changing the amount of aluminum in the metalized glass layer.
The specific data is subject to PDF, and the above content is for reference
| Part Number | Manufacturer | Price | Quantity | Description |
|---|
| CF14JA91K0 | Stackpole El... | 0.01 $ | 1000 | RES 91K OHM 1/4W 5% AXIAL... |
| CF14GT3K90 | Stackpole El... | 0.01 $ | 1000 | RES 3.9K OHM 1/4W 2% AXIA... |
| CF14GT9K10 | Stackpole El... | 0.01 $ | 1000 | RES 9.1K OHM 1/4W 2% AXIA... |
| CF14JT18K0 | Stackpole El... | 0.0 $ | 60000 | RES 18K OHM 1/4W 5% AXIAL... |
| CF14JA12K0 | Stackpole El... | 0.01 $ | 1000 | RES 12K OHM 1/4W 5% AXIAL... |
| CF14JA130R | Stackpole El... | 0.01 $ | 1000 | RES 130 OHM 1/4W 5% AXIAL... |
| CF14JA6K80 | Stackpole El... | 0.01 $ | 1000 | RES 6.8K OHM 1/4W 5% AXIA... |
| CF14GT430K | Stackpole El... | 0.01 $ | 1000 | RES 430K OHM 1/4W 2% AXIA... |
| CF14JA68K0 | Stackpole El... | 0.01 $ | 1000 | RES 68K OHM 1/4W 5% AXIAL... |
| CF14GT15K0 | Stackpole El... | 0.01 $ | 1000 | RES 15K OHM 1/4W 2% AXIAL... |
| CF14JT160K | Stackpole El... | 0.0 $ | 5000 | RES 160K OHM 1/4W 5% AXIA... |
| CF14JB9M10 | Stackpole El... | 0.01 $ | 1000 | RES 9.1M OHM 1/4W 5% AXIA... |
| CF14JA7M50 | Stackpole El... | 0.01 $ | 1000 | RES 7.5M OHM 1/4W 5% AXIA... |
| CF14JT180R | Stackpole El... | 0.0 $ | 65000 | RES 180 OHM 1/4W 5% AXIAL... |
| CF14JT68R0 | Stackpole El... | 0.0 $ | 45000 | RES 68 OHM 1/4W 5% AXIAL6... |
| CF14JA5R60 | Stackpole El... | 0.01 $ | 1000 | RES 5.6 OHM 1/4W 5% AXIAL... |
| CF14JA13K0 | Stackpole El... | 0.01 $ | 1000 | RES 13K OHM 1/4W 5% AXIAL... |
| CF14GT22R0 | Stackpole El... | 0.01 $ | 1000 | RES 22 OHM 1/4W 2% AXIAL2... |
| CF14JT10R0 | Stackpole El... | 0.0 $ | 115000 | RES 10 OHM 1/4W 5% AXIAL1... |
| CF14JT18R0 | Stackpole El... | 0.0 $ | 40000 | RES 18 OHM 1/4W 5% AXIAL1... |
| CF14JA11K0 | Stackpole El... | 0.01 $ | 1000 | RES 11K OHM 1/4W 5% AXIAL... |
| CF14JA180K | Stackpole El... | 0.01 $ | 1000 | RES 180K OHM 1/4W 5% AXIA... |
| CF14JA200R | Stackpole El... | 0.01 $ | 1000 | RES 200 OHM 1/4W 5% AXIAL... |
| CF14GT10R0 | Stackpole El... | 0.01 $ | 1000 | RES 10 OHM 1/4W 2% AXIAL1... |
| CF14GT240R | Stackpole El... | 0.01 $ | 1000 | RES 240 OHM 1/4W 2% AXIAL... |
| CF14JT56R0 | Stackpole El... | 0.0 $ | 40000 | RES 56 OHM 1/4W 5% AXIAL5... |
| CF14JT150K | Stackpole El... | 0.0 $ | 5000 | RES 150K OHM 1/4W 5% AXIA... |
| CF14JT3M90 | Stackpole El... | 0.0 $ | 10000 | RES 3.9M OHM 1/4W 5% AXIA... |
| CF14GT150R | Stackpole El... | 0.01 $ | 1000 | RES 150 OHM 1/4W 2% AXIAL... |
| CF14GT36K0 | Stackpole El... | 0.01 $ | 1000 | RES 36K OHM 1/4W 2% AXIAL... |
| CF14JB43K0 | Stackpole El... | 0.01 $ | 1000 | RES 43K OHM 1/4W 5% AXIAL... |
| CF14JT1M50 | Stackpole El... | 0.0 $ | 40000 | RES 1.5M OHM 1/4W 5% AXIA... |
| CF14JT7K50 | Stackpole El... | 0.0 $ | 30000 | RES 7.5K OHM 1/4W 5% AXIA... |
| CF14JT270K | Stackpole El... | 0.0 $ | 30000 | RES 270K OHM 1/4W 5% AXIA... |
| CF14JT30R0 | Stackpole El... | 0.0 $ | 10000 | RES 30 OHM 1/4W 5% AXIAL3... |
| CF14JT1M30 | Stackpole El... | 0.05 $ | 4750 | RES 1.3M OHM 1/4W 5% AXIA... |
| CF14JT820K | Stackpole El... | 0.0 $ | 1000 | RES 820K OHM 1/4W 5% AXIA... |
| CF14JT1R80 | Stackpole El... | 0.01 $ | 1000 | RES 1.8 OHM 1/4W 5% AXIAL... |
| CF14JT91R0 | Stackpole El... | 0.05 $ | 17757 | RES 91 OHM 1/4W 5% AXIAL9... |
| CF14JA5R10 | Stackpole El... | 0.0 $ | 1000 | RES 5.1 OHM 1/4W 5% AXIAL... |
RES WW 7W 5% TH68 kOhms 5% 7W Through Ho...
RES WW 7W 5% TH1.3 Ohms 5% 7W Through Ho...
RES 24.9 OHM 1/4W 1% AXIAL24.9 Ohms 1% 0...
RES 2.8 OHM 3W 0.5% WW AXIAL2.8 Ohms 0.5...
RES 750K OHM 1/4W 1% AXIAL750 kOhms 1% 0...
RES 340 OHM 1W 1% WW AXIAL340 Ohms 1% 1W...
CF14JB390K Datasheet/PDF