Allicdata Part #: | 909-1037-2-ND |
Manufacturer Part#: |
RFCS04021000CBTT1 |
Price: | $ 0.00 |
Product Category: | Capacitors |
Manufacturer: | Vishay Electro-Films |
Short Description: | CAP SILICON 1PF 50V 0402 |
More Detail: | 1pF Silicon Capacitor 50V 0402 (1005 Metric) |
DataSheet: | RFCS04021000CBTT1 Datasheet/PDF |
Quantity: | 1000 |
Lead Free Status / RoHS Status: | Lead free / RoHS Compliant |
Moisture Sensitivity Level (MSL): | 1 (Unlimited) |
1 +: | 0.00000 |
Series: | RFCS |
Packaging: | Tape & Reel (TR) |
Lead Free Status / RoHS Status: | -- |
Part Status: | Obsolete |
Moisture Sensitivity Level (MSL): | -- |
Capacitance: | 1pF |
Tolerance: | ±0.1pF |
Voltage - Breakdown: | 50V |
ESL (Equivalent Series Inductance): | -- |
Applications: | -- |
Features: | -- |
Operating Temperature: | -55°C ~ 125°C |
Package / Case: | 0402 (1005 Metric) |
Height: | 0.016" (0.41mm) |
Size / Dimension: | 0.040" L x 0.020" W (1.02mm x 0.51mm) |
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Silicon Capacitors are an essential component in many electronics and engineering designs. They are generally used for storing or changing electric energy and providing a conductive path for electric signals. RFCS04021000CBTT1 is a type of silicon capacitor with an application field and working principle that sets it apart from other types in the industry.
A silicon capacitor is an electrical device made up of two overlapping conductive plates, separated by a non-conducting dielectric material. These plates, or electrodes, are connected together and form a capacitor. In the case of RFCS04021000CBTT1, the plates are made up of a polymer-based material with a metal electrode pattern. This type of capacitor is distinct from other types because the polymer-based material makes it much more flexible and durable than conventional ones.
The RFCS04021000CBTT1 is most often used in pulse applications, such as in audio and video signal processing. Its low ESR and capacitance values make it ideal for high-frequency processes where voltage fluctuations occur quickly and frequently. In terms of its application field, it is known for its high-frequency or long-term operation stability. Its use in radio frequency applications, such as television, wireless communication systems and radar, means that it can handle both low- and high-frequency signals.
The working principle of the RFCS04021000CBTT1 is based on the electric field generated between the capacitor’s two batteries. When an electric current passes through the electrodes, it charges them. The dielectric material between the charged electrodes stores energy in the form of an electric field. If the dielectric material is of a high-quality, then this electric field can be maintained for a longer period of time.
The RFCS04021000CBTT1 also offers higher capacitance when compared to other conventional capacitors. This can be beneficial when dealing with a large number of signals because higher capacitance allows for less energy being used up during the capacitor’s operation. The increased stability of the RFCS04021000CBTT1 also makes it beneficial when dealing with electric signals in high-voltage applications or covering vast frequencies.
In addition to its high-frequency operation stability, the RFCS04021000CBTT1 also comes with an extremely high isolation rate. This means that it can safely store charge even when high voltage levels are present, a crucial feature for use in sensitive applications. Its high resistance to temperature, humidity, and mechanical stress also make it a much more reliable choice than other traditional capacitors.
The unique application field and working principle of the RFCS04021000CBTT1 make it an ideal choice for pulse applications and high-frequency AC circuits. Its flexibility and durability, along with its high capacitance, isolation rate and resistance to temperature, humidity, and mechanical stress, make it an invaluable part of the electronic industry.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
RFCS04026000DBTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 0.6PF 50V 040... |
RFCS04027000DBTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 0.7PF 50V 040... |
RFCS04028000DBTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 0.8PF 50V 040... |
RFCS04026000DBTTS | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 0.6PF 50V 040... |
RFCS04029000DBTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 0.9PF 50V 040... |
RFCS04024700CJTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 4.7PF 5% 25V ... |
RFCS04027000DBTTS | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 0.7PF 50V 040... |
RFCS04025600CJTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 5.6PF 5% 25V ... |
RFCS04028000DBTTS | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 0.8PF 50V 040... |
RFCS04026800CJTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 6.8PF 5% 25V ... |
RFCS04028200CJTTS | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 8.2PF 5% 25V ... |
RFCS04028200CJTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 8.2PF 5% 25V ... |
RFCS04029000DBTTS | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 0.9PF 50V 040... |
RFCS04025000DBTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 0.5PF 50V 040... |
RFCS04022000DBTTS | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 0.2PF 50V 040... |
RFCS04024000DBTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 0.4PF 50V 040... |
RFCS04022200BJTTS | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 22PF 5% 10V 0... |
RFCS04022200CJTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 2.2PF 5% 50V ... |
RFCS04022700CJTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 2.7PF 5% 50V ... |
RFCS04022700BJTTS | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 27PF 5% 10V 0... |
RFCS04023300CJTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 3.3PF 5% 25V ... |
RFCS04022700CJTTS | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 2.7PF 5% 50V ... |
RFCS04023900CJTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 3.9PF 5% 25V ... |
RFCS04023000DBTTS | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 0.3PF 50V 040... |
RFCS04022200BJTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 22PF 5% 10V 0... |
RFCS04022700BJTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 27PF 5% 10V 0... |
RFCS04023900CJTTS | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 3.9PF 5% 25V ... |
RFCS04024000DBTTS | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 0.4PF 50V 040... |
RFCS04023000DBTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 0.3PF 50V 040... |
RFCS04021200BJTTS | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 12PF 5% 16V 0... |
RFCS04021200CBTTS | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 1.2PF 50V 040... |
RFCS04021500BJTTS | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 15PF 5% 16V 0... |
RFCS04021800CBTTS | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 1.8PF 50V 040... |
RFCS04022000DBTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 0.2PF 50V 040... |
RFCS04021000CBTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 1PF 50V 04021... |
RFCS04021200CBTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 1.2PF 50V 040... |
RFCS04021500CBTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 1.5PF 50V 040... |
RFCS04021800CBTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 1.8PF 50V 040... |
RFCS04021000BJTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 10PF 5% 25V 0... |
RFCS04021200BJTT1 | Vishay Elect... | 0.0 $ | 1000 | CAP SILICON 12PF 5% 16V 0... |
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