
Allicdata Part #: | BFC2370GC681-ND |
Manufacturer Part#: |
BFC2370GC681 |
Price: | $ 0.07 |
Product Category: | Capacitors |
Manufacturer: | Vishay BC Components |
Short Description: | CAP FILM 680PF 5% 630VDC RADIAL |
More Detail: | 680pF Film Capacitor 220V 630V Polyester, Metalliz... |
DataSheet: | ![]() |
Quantity: | 1000 |
Moisture Sensitivity Level (MSL): | 1 (Unlimited) |
Lead Free Status / RoHS Status: | Lead free / RoHS Compliant |
1500 +: | $ 0.06151 |
Operating Temperature: | -55°C ~ 105°C |
Features: | Long Life |
Ratings: | AEC-Q200 |
Applications: | Automotive |
Lead Spacing: | 0.200" (5.08mm) |
Termination: | PC Pins |
Height - Seated (Max): | 0.315" (8.00mm) |
Size / Dimension: | 0.283" L x 0.138" W (7.20mm x 3.50mm) |
Package / Case: | Radial |
Mounting Type: | Through Hole |
Series: | MKT370 |
Dielectric Material: | Polyester, Metallized |
Voltage Rating - DC: | 630V |
Voltage Rating - AC: | 220V |
Tolerance: | ±5% |
Capacitance: | 680pF |
Moisture Sensitivity Level (MSL): | -- |
Part Status: | Active |
Lead Free Status / RoHS Status: | -- |
Packaging: | Tape & Box (TB) |
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Film capacitors, also known as plastic film capacitors, are electronic components consisting of two electrical conductors separated by a dielectric film. The BFC2370GC681 is a film capacitor designed and manufactured by Shanghai Eling Electronics Co., Ltd. This capacitor is widely used in many applications due to its superior performance, reliability and long-term stability. This article explores the application field and working principle of the BFC2370GC681 capacitor.
The BFC2370GC681 is a general-purpose surface-mount film capacitor. It is typically used in the conditioning of power supplies and other power-line circuits, high-voltage direct current (D-C) applications, and for RFI/EMI noise suppression. In these applications, the capacitor helps to reduce transients, minimize EMI-radiated noise, and provide effective decoupling. This makes it ideal for use in power line filtering, power supply filtering, and motor drive circuits. The low ESR and high-temperature rating of the BFC2370GC681 make it suitable for harsh environments and industrial applications. Additionally, its superior capacitance stability and low-loss characteristics make it ideal for use in a wide range of applications such as audio amplification, RF amplifiers, cellular telephones, portable electronic devices, and other electronic devices. These features make the BFC2370GC681 an excellent choice for high-reliability applications.
The BFC2370GC681 has a working voltage of 250V and a rated temperature of -55°C to +150°C. It is made from a high-performance metallized polypropylene film, ensuring that the capacitor has a low loss, low ESR, excellent stability under temperature and frequency, high insulation resistance, reliable temperature characteristics, and good frequency characteristics. Furthermore, the capacitor has a capacitance of 0.033μF-2.2μF, a tolerance of ±5%, and a working frequency of up to 250V DC.
The working principle of the BFC2370GC681 is based on the capacitor storing charge when there is a potential difference between the two terminals. This potential difference creates an electric field across the dielectric film, which polarizes the charges and an electric field or electrostatic field is generated. The capacitance of the capacitor is then determined by the ratio of the electric field to the potential difference between the two terminals. The higher this ratio, the higher the capacitance.
In conclusion, the BFC2370GC681 is a general-purpose film capacitor that is suitable for a wide range of applications including power line filtering, power supply filtering, and motor drive circuits. Due to its low loss, low ESR, excellent stability, high insulation resistance, and good frequency characteristics, the BFC2370GC681 is an excellent choice for high-reliability applications. Furthermore, its working principle is based on the capacitor storing charge when there is a potential difference between the two terminals, and the capacitance of the capacitor is determined by the ratio of the electric field to the potential difference between the two terminals.
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