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Controlling Angular Deviation in Permanent Magnets Through Data-Driven Manufacturing
2025/07/11 Min Zou

Angular Deviation (θz) in Permanent Magnet is defined as the angle between a magnet's internal magnetization direction and its geometric reference axis (e.g., designated surface or centerline).

Sintered NdFeB magnets typically exhibit θz between 0° and 7°, with ≤5° being a common production tolerance.

Why This Matters

Even a small angular deviation can cause significant magnetic field distortion:  

-    ⬇️ Reduced normal field component (Bz)

-    ⬆️ Increased in-plane components (Bx, By)     

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If field deviation exceeds just a few percent, precision applications, such as sensors, medical devices, and actuators, are at risk of critical performance degradation.

This article explores how angular deviation develops during manufacturing, what our data shows about spatial trends, and what manufacturers can do to control it.


What the Data Shows: Spatial Variations Are Real

We conducted an analysis of angular deviation in a sintered NdFeB magnet block. The block dimensions were 34 × 50.7 × 43.7 mm,    with    the following sampling details:

50.7 mm corresponds to the non-pressed, non-oriented direction. After grinding off 0.6 mm, three slices were taken from the front, center, and rear, each 1.73 mm thick, corresponding to spatial    coordinates X1, X2, X3.

43.7 mm is the pressing direction. After grinding off 0.6 mm, three slices were taken from the top, center, and bottom, each 6.845 mm thick, corresponding to Y1, Y2, Y3, with Y3 being the pressed bottom surface.

34 mm is the orientation direction. After removing 0.6 mm from the surface, 20 layers were sliced at 1.3 mm intervals, corresponding to spatial coordinates Z1 through Z20In total, 180 sampling positions were measured for angular deviation, and the resulting data was used to analyze the spatial distribution of angular deviation within the block.

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The results revealed clear spatial patterns in angular deviation.

Along the Non-pressed, Non-Oriented (X)
Direction:

- No obvious trend

Along the Pressing (Y) Direction:  

- The bottom surface (Y3) has θz 35%
higher than the top surface            (Y1)  

Across the oriented (Z) axis:

- Center layers (Z10) show θz less than 2°

- Edge layers (Z1 and Z20) reach over 4° 

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2D          Contour          Mapping across all planes confirm a gradual shift in θz  across all planes – highlighting the          cumulative impact of process variation.  

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What’s Causing the Deviation

Several steps in the manufacturing process can introduce angular deviation. Here are the key contributors:

Stage

What Happens

Effect on θz
Orientation Pressing Non-uniform particle alignment Baseline deviation of 0.5°- 2°
Isostatic Pressing Density shifts and deformation Adds ~0.5°
Sintering Anisotropic shrinkage (20% axial vs. 5% radial) Sustains 0.5°- 2°baseline
Machining Fixture misalignment Adds another 0.5 - 2° 


How We Can Reduce θz: Actionable Solutions

Based on our findings, here are three strategies that show promise:

1. Mold Calibration with Isotropic Materials

· Calibration using isotropic materials can verify that the magnetic field aligns perpendicular to the intended magnetization    direction.  

2. Design Adjustments  

· Shorten the pressing (Y) axis to reduce powder settling

· Widen the non-oriented (X) axis size to reduce deformation risk  

3. Streamline the Process

· Eliminating isostatic pressing can help reduce handling deformation   


The Goal: θz ≤ 3°

By implementing these strategies, we estimate a 40% improvement in angular deviation, reducing θz to 3° or less — a level that significantly enhances magnetic field quality in precision applications.

We’ll be publishing our data after implementing these strategies in Q3 2025—stay tuned!


### APPENDIX:    Angular Deviation Testing Methodologies

Technical Principles for Engineering Teams 

Method Core Principle Key Specifications

Helmholtz Coil

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Measure the magnetic dipole moment components in three

mutually orthogonal directions to compute the magnetic moment orientation

GR&R: 3% · Cycle time: 5s · Max sample dimension: Determined by the coil diameter

MagCheck
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6-DOF inverse field modeling to compute magnetic moment vector GR&R: 6% · Cycle time: 6s · Rectangular magnets: Maximum dimension ≤ 80 mm

Cylindrical/Ring magnets: Diameter ≤ 100 mm, Height ≤ 50 mm

MagCam
10

Hall sensor array + Bz inversion to map surface magnetization vectors Resolution: 3% · Cycle time: 20s ·Max sample dimension: 12.7 x 12.7 mm

Why Helmholtz Coil Was Chosen:  

- Scalability: Cost-effective for mass production environments

- Reproducibility: Achieves 3% accuracy across different lab setups  

- Practicality: Supports production-sized samples


Access NdFeB Permanent Magnet Material Property Datasheets 

· Sintered NdFeB Magnets

· Bonded NdFeB Magnets


Try Our Magnetic Calculator

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