Insulation Design

Category: Electromagnetic Field Analysis | Consolidated Edition 2026-04-06
CAE visualization for insulation design theory - technical simulation diagram
Insulation Design

Insulation Design: Theoretical Foundations

Approach to Insulation Design

🧑🎓

Professor, is insulation design essentially about "keeping the electric field below the dielectric strength"?


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Exactly. The design flow is:


1. Determine electrode shape and insulation configuration

2. Calculate electric field distribution using FEM

3. Verify that the maximum electric field $E_{max}$ is below the dielectric strength $E_b$ of each material

4. Evaluate the safety factor $SF = E_b / E_{max}$


Electric Field Mitigation Techniques

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TechniquePrincipleApplication Example
Fillet (Rounding)Increase the curvature radius of edges to mitigate electric field concentrationHigh-voltage electrodes
Corona RingEnlarge the equipotential surface to homogenize the electric fieldTransmission line insulators
Stress ConePush out the electric field using high-permittivity materialCable terminations
Shield ElectrodeShield the electric field with a grounded electrodeGIS (Gas Insulated Switchgear)
Graded InsulationGradually change the $\varepsilon_r$ (relative permittivity)Bushings

Summary

🎓
  • $E_{max} < E_b / SF$ — Fundamental condition for insulation design
  • Electric Field Mitigation — Fillet, corona ring, stress cone
  • Predict electric field distribution with FEM — Optimization of design

Coffee Break Yomoyama Talk

The Dawn of Insulation Engineering—The History of Cable Insulation and Gutta-Percha (1850s)

The engineering use of electrical insulating materials began in the 1850s during the era of submarine cable laying. When the Dover Strait submarine cable connecting England and France was laid in 1851, a natural rubber from Malaysia called "Gutta-percha" was used as the insulating material. However, the first transatlantic cable (1858) failed due to insulation breakdown after just three weeks—insulation engineering at the time relied solely on empirical rules. Subsequently, the electric line of force theory, which evolved from Coulomb's law (1785), was systematized by Maxwell (1873), establishing the foundation for modern electric field analysis. Today's FEM electric field analysis solves Maxwell's equations through discretization, with theories from 170 years ago forming the mathematical basis for cutting-edge insulation design tools.

Computational Methods for Insulation Design

FEM Flow for Insulation Design

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1. CAD Model Construction (Electrodes + Insulators + Surrounding Space)

2. Material Settings ($\varepsilon_r$ for each region)

3. Boundary Conditions (Electrode potential, ground, symmetry plane)

4. Mesh (Refine areas of electric field concentration)

5. Solve (Laplace/Poisson equation)

6. Postprocessing ($E_{max}$, safety factor map)


🧑🎓

How does mesh coarseness affect the results?


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The electric field has high mesh dependency (derivative of potential). Place at least 4–6 layers of elements at electrode edges. Second-order elements are recommended.


Summary

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  • Mesh quality in electric field concentration areas is key
  • Ensure electric field accuracy with second-order elements
  • Visualize design margin with safety factor maps

Coffee Break Yomoyama Talk

FEM Analysis of Solid Insulation—Mesh Refinement and Convergence Verification of Electric Field Concentration Factor

In FEM electric field analysis of solid insulating materials (epoxy, XLPE, ceramic), electric field concentration occurs at shape corners, edges, and electrode ends. Mesh refinement in these concentrated areas is crucial for accuracy. Practical procedure for verifying electric field convergence: ① Analyze the target area with three mesh levels (coarse, medium, fine) and judge convergence when the change rate of the maximum electric field value is below 1%. ② Set the minimum mesh size to R/20 or less relative to the edge curvature radius R (e.g., mesh ≤5um for R=0.1mm). ③ At interfaces where the relative permittivity ratio (er) differs significantly (e.g., air er=1 vs. epoxy er=4), the electric field changes abruptly due to discontinuity in normal electric flux density, so ensure equally dense meshes on both sides of the interface. Underestimating the electric field concentration factor Kt by more than 3% risks insufficient design safety factor in actual equipment.

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