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ADP1031ACPZ-3-R7 bảng dữ liệu(PDF) 34 Page - Analog Devices |
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ADP1031ACPZ-3-R7 bảng dữ liệu(HTML) 34 Page - Analog Devices |
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34 / 38 page ![]() ADP1031 Data Sheet Rev. A | Page 34 of 38 INSULATION LIFETIME All insulation structures eventually break down when subjected to voltage stress over a sufficiently long period. The rate of insulation degradation is dependent on the characteristics of the voltage waveform applied across the insulation as well as on the materials and material interfaces. The two types of insulation degradation of primary interest are breakdown along surfaces exposed to the air and insulation wear out. Surface breakdown is the phenomenon of surface tracking and the primary determinant of surface creepage requirements in system level standards. Insulation wear out is the phenomenon where charge injection or displacement currents inside the insulation material cause long-term insulation degradation. Surface Tracking Surface tracking is addressed in electrical safety standards by setting a minimum surface creepage based on the working voltage, the environmental conditions, and the properties of the insulation material. Safety agencies perform characterization testing on the surface insulation of components that allows the components to be categorized in different material groups. Lower material group ratings are more resistant to surface tracking. Therefore, lower material group ratings provide adequate lifetime with smaller creepage. The minimum creepage for a given working voltage and material group is determined in each system level standard and is based on the total rms voltage across the isolation, pollution degree, and material group. The material group and creepage for the ADP1031 isolators are shown in Table 4. Insulation Wear Out The lifetime of insulation is determined by thickness, material properties, and the voltage stress applied. It is important to verify that the product lifetime is adequate at the application working voltage. The working voltage supported by an isolator for wear out may not be the same as the working voltage supported for tracking. The working voltage applicable to tracking is specified in most standards. Testing and modeling have shown that the primary driver of long-term degradation is displacement current in the polyimide insulation. This displacement current causes incremental damage to the insulation. The stress on the insulation can be broken down into broad categories: dc stress and ac component time varying voltage stress. DC stress causes very little insulation wear out because there is no displacement current. AC component time varying voltage stress causes insulation wear out. The ratings in certification documents are usually based on 60 Hz sinusoidal stress because this reflects isolation from line voltage. However, many practical applications have combinations of 60 Hz ac and dc across the barrier as shown in Equation 1. Because only the ac portion of the stress causes wear out, the equation can be rearranged to solve for the ac rms voltage, as shown in Equation 2. For insulation wear out with the polyimide materials, the ac rms voltage determines the product lifetime. 2 2 DC RMS AC RMS V V V + = (1) or 22 AC RMS RMS DC V V V = − (2) where: VRMS is the total rms working voltage. VAC RMS is the time varying portion of the working voltage. VDC is the dc offset of the working voltage. Calculation and Use of Parameters Example The following example frequently arises in power conversion applications. Assume that the line voltage on one side of the isolation is 240 V ac rms and a 400 V dc bus voltage is present on the other side of the isolation barrier. The isolator material is polyimide. To establish the critical voltages in determining the creepage, clearance, and lifetime of a device, see Figure 75 and the following equations. TIME VAC RMS VRMS VDC VPEAK Figure 75. Critical Voltage Example The working voltage across the barrier from Equation 1 is 2 2 DC RMS AC RMS V V V + = 2 2 400 240 + = RMS V VRMS = 466 V This VRMS value is the working voltage and is used together with the material group and pollution degree when looking up the creepage required by a system standard. To determine if the lifetime is adequate, obtain the time varying portion of the working voltage. To obtain the ac rms voltage, use Equation 2. 22 AC RMS RMS DC V V V = − 2 2 400 466 − = RMS AC V VAC RMS = 240 V rms In this case, the ac rms voltage is simply the line voltage of 240 V rms. This calculation is more relevant when the waveform is not sinusoidal. The value is compared to the limits for working voltage in Table 8 for the expected lifetime, which is less than a |
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