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A Revolution in Dielectric Materials: The Evolution of High-Voltage Capacitors from Basic Insulation to Intelligent Response
 
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x| Menghilangnya | ≦0,0040 | menahan tegangan | 1.5ur ● 1 menit | 
|---|---|---|---|
| tegangan Resistansi isolasi | ≧ 1.0 × 105mΩ | 
A Revolution in Dielectric Materials: The Evolution of High-Voltage Capacitors from Basic Insulation to Intelligent Response
Drawing:
Parameters:
| No. | Specification | Dissipation | Withstanding voltage | Insulation resistance | Dimension(mm) | ||||
| 1 | 20kV-2000pF | ≦0.0040 | 1.5Ur● 1min | ≧1.0×105MΩ | D | H | L | D | M | 
| 2 | 20kV-10000pF | 45 | 19 | 23 | 12 | 5 | |||
| 3 | 20kV-18000pF | 65 | 15 | 19 | 12 | 5 | |||
| 4 | 30kV-1000pF | 80 | 17 | 25 | 12 | 5 | |||
| 5 | 30kV-2700pF | 45 | 24 | 32 | 12 | 4 | |||
| 6 | 30kV-12000pF | 60 | 20 | 28 | 12 | 4 | |||
| 7 | 40kV-150pF | 20 | 33 | 41 | 8 | 4 | |||
| 8 | 40kV-500pF | 28 | 33 | 41 | 8 | 4 | |||
| 9 | 40kV-7500pF | 80 | 24 | 29 | 12 | 6 | |||
| 10 | 40kV-10000pF | 80 | 22 | 26 | 16 | 5 | |||
| 11 | 50kV-1000pF | 50 | 30 | 34 | 12 | 4 | |||
| 12 | 50kV-1000pF | 32 | 27 | 31 | 16 | 5 | |||
| 13 | 50kV-5600pF | 80 | 31 | 35 | 16 | 5 | |||
| 14 | 60kV-1500pF | 50 | 31 | 34 | 12 | 5 | |||
| 15 | 60kV-3000pF | 65 | 32 | 35 | 16 | 5 | |||
| 16 | 100kV-500pF | 50 | 54 | 58 | 12 | 5 | |||
| 17 | 100kV-2000pF | 51 | 32 | 35 | 16 | 5 | |||
| 18 | Insulator type 100kV-1500pF | 68 | 36 | 40 | 16 | 5 | |||
| 19 | 150kV-820pF | 65 | 95 | 100 | 12 | 5 | |||
| 20 | 200kV-600pF | 50 | 90 | 94 | 16 | 5 | |||
The core competitiveness of high-voltage doorknob capacitors stems from breakthroughs in dielectric materials. We've abandoned traditional single-material systems and developed a nanocomposite dielectric with adaptive properties, evolving capacitors from passive energy storage elements to intelligently responsive system optimizers.
Our third-generation dielectric material, by incorporating functionalized nanofillers into a barium strontium titanate matrix, achieves three major breakthroughs: First, a three-dimensionally stable dielectric constant-temperature-frequency relationship is established, enabling the capacitance temperature coefficient to be controlled within ±15ppm/°C from -40°C to 125°C. Second, through precise control of interfacial polarization, dielectric loss is reduced to 5×10⁻⁵ at 1MHz. Most importantly, the material exhibits self-healing properties, automatically repairing microscopic defects in the event of localized overvoltage, extending the product's service life to more than three times that of conventional products.
This material innovation brings significant system-level benefits: in PLC systems in coastal areas, our capacitors demonstrate excellent moisture and corrosion resistance; in inland areas with large temperature differences, system communication quality is no longer affected by temperature changes; and in complex industrial power environments, the linearity exhibited by the capacitors ensures the fidelity of signal transmission over a large dynamic range.
 


 
                         
                         
                        