Mutual Inductance Calculation Using Dipole Approximation

Resolve Bottlenecks,
Find Innovative Solutions
Generate Solutions

Solution Overview

Problem

Current methods for analyzing mutual inductance in high-frequency integrated circuits are computationally expensive and inefficient, particularly when dealing with close-spaced intentional inductors, leading to challenges in noise analysis and design optimization.

Innovation Solution

The use of a dipole approximation technique to calculate mutual inductance, which simplifies the computation by representing magnetic fields as those generated by a dipole moment, reducing computational complexity and allowing for efficient noise analysis and design exploration across various layouts, including non-Manhattan configurations.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If conventional methods are used to calculate mutual inductance, then accuracy is maintained, but computational complexity increases significantly

Engineering Contradiction:
Improvemutual inductance calculation accuracyVSAvoidcomputational complexity
Core Design Contradiction:
Measurement precisionVSDevice complexity

Solution Approach 1:

The patent segments the inductor structures into discrete geometric components (rectangles, polygons) and calculates mutual inductance by summing contributions from individual segment pairs. This segmentation allows the use of simplified analytical formulas for each segment while maintaining overall accuracy, reducing computational complexity from O(N²) to O(N) where N is the number of segments.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The patent introduces an intermediary computational approach using analytical formulas based on geometric parameters (area, perimeter, separation distance) rather than direct numerical integration of magnetic fields. This intermediary method provides accurate results with significantly reduced computational effort compared to conventional full-wave electromagnetic simulations.

Inventive Principle:
Principle #24Intermediary (Mediator)

2Area of stationary object

If inductors are spaced closely together to minimize area, then area occupation is reduced, but noise and cross talk increase

Engineering Contradiction:
Improvelayout areaVSAvoidelectromagnetic noise
Core Design Contradiction:
Area of stationary objectVSObject-affected harmful factors

Solution Approach 1:

The patent implements a feedback mechanism where the calculated mutual inductance values are used to evaluate noise coupling between adjacent inductors. The design tool iteratively adjusts inductor spacing and orientation based on the calculated noise levels, allowing designers to find optimal configurations that minimize area while maintaining acceptable noise margins through quantitative feedback.

Inventive Principle:
Principle #23Feedback

Solution Approach 2:

The patent enables parameter changes in the inductor design by allowing adjustment of geometric parameters (width, length, spacing, orientation) and calculating their impact on mutual inductance. This allows systematic optimization of layout parameters to achieve the desired trade-off between area efficiency and noise performance.

Inventive Principle:
Principle #35Parameter changes

3Measurement precision

If conventional computational methods are used for noise analysis, then accuracy is maintained, but design exploration time increases

Engineering Contradiction:
Improvenoise analysis accuracyVSAvoiddesign exploration time
Core Design Contradiction:
Measurement precisionVSLoss of time

Solution Approach 1:

The patent performs preliminary calculation of geometric parameters (area, perimeter, centroid positions) for all inductor structures before conducting mutual inductance analysis. This preliminary action prepares the necessary geometric data in advance, enabling rapid noise analysis without repeated geometric computations during design exploration iterations.

Inventive Principle:
Principle #10Preliminary action

Solution Approach 2:

The patent uses simplified analytical models that copy the essential geometric characteristics of complex inductor structures without requiring full electromagnetic field simulations. This copying approach maintains sufficient accuracy for noise analysis while dramatically reducing computational time, enabling rapid design space exploration.

Inventive Principle:
Principle #26Copying

Applied Scientific Principles

This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.

Function Achieved in This Case

This approach significantly reduces computational complexity, enabling faster and more accurate noise analysis and design optimization for high-frequency circuits, while allowing for flexible layout configurations that minimize area occupation while meeting noise limits.

Implementation Method 1

representing magnetic fields as those generated by a dipole moment

Methodology Applied
Scientific EffectMagnetic field: Magnetic Field

Implementation Method 2

calculate mutual inductance

Methodology Applied
Scientific EffectElectromagnetic induction: Electromagnetic Induction

Data Source

PatentUS8161438B2Determining mutual inductance between intentional inductors
Publication Date: 2012.04.17 SIEMENS INDUSTRY SOFTWARE INC
  • US8161438B2 patent drawing
  • US8161438B2 patent drawing
  • US8161438B2 patent drawing

AI summary

Various methods for analyzing mutual inductance in an integrated circuit layout are disclosed. In one exemplary embodiment, for example, circuit design information indicative of a first inductor and a second inductor is received. A dipole moment associated with the first inductor is determined, where the magnetic field associated with the dipole moment is representative of magnetic fields created by respective turns in the first inductor. A mutual inductance between the first inductor and the second inductor is determined by determining a magnetic flux of the magnetic field of the dipole moment through surfaces bounded by respective wire segments of the second inductor.