MP 62x42x25 / N38 - ring magnet
ring magnet
Catalog no 030205
GTIN/EAN: 5906301812227
- Diameter
- 62 mm [±0,1 mm]
- internal diameter Ø
- 42 mm [±0,1 mm]
- Height
- 25 mm [±0,1 mm]
- Weight
- 306.31 g
- Magnetization Direction
- ↑ axial
- Coating
- [NiCuNi] Nickel
How we measure these parameters — certificates and measurements
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Engineering report for this magnet
Full PDF analysis: pull and shear force, effect of distance, temperature and plate thickness, safety distances and the demagnetization curve.
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Technical data - MP 62x42x25 / N38 - ring magnet
Specification / characteristics - MP 62x42x25 / N38 - ring magnet
| properties | values |
|---|---|
| Cat. no. | 030205 |
| GTIN/EAN | 5906301812227 |
| Distributor | Dhit sp. z o.o. |
| Country of origin | Poland / China / Germany |
| Customs code | 85059029 |
| Diameter | 62 mm [±0,1 mm] |
| internal diameter Ø | 42 mm [±0,1 mm] |
| Height | 25 mm [±0,1 mm] |
| Weight | 306.31 g |
| Magnetization Direction | ↑ axial |
| Load capacity ~ ? | 58.67 kg / 575.60 N |
| Magnetic Induction ~ ? | 389.14 mT / 3891 Gs |
| Coating | [NiCuNi] Nickel |
| Manufacturing Tolerance | ±0.1 mm |
Magnetic properties of material N38
| properties | values | units |
|---|---|---|
| Remanence Br ? | 12.2-12.6 | kGs |
| Remanence Br ? | 1220-1260 | mT |
| Coercivity bHc ? | 10.8-11.5 | kOe |
| Coercivity bHc ? | 860-915 | kA/m |
| Intrinsic coercivity iHc | ≥ 12 | kOe |
| Intrinsic coercivity iHc | ≥ 955 | kA/m |
| Energy product BHmax ? | 36-38 | BH max MGOe |
| Energy product BHmax ? | 287-303 | BH max KJ/m |
| Maximum working temperature ? | ≤ 80 | °C |
Physical properties of sintered neodymium magnets Nd2Fe14B at 20°C
| properties | values | units |
|---|---|---|
| Vickers hardness | ≥550 | Hv |
| Density | ≥7.4 | g/cm3 |
| Curie Temperature TC | 310 | °C |
| Curie Temperature TF | 590 | °F |
| Specific resistance | 150 | μΩ⋅cm |
| Bending strength | 250 | MPa |
| Compressive strength | 1000~1100 | MPa |
| Thermal expansion parallel (∥) to orientation (M) | (3-4) x 10-6 | °C-1 |
| Thermal expansion perpendicular (⊥) to orientation (M) | -(1-3) x 10-6 | °C-1 |
| Young's modulus | 1.7 x 104 | kg/mm² |
Engineering modeling of the magnet - data
Presented values represent the outcome of a mathematical calculation. Values were calculated on algorithms for the class Nd2Fe14B. Operational parameters might slightly differ. Use these calculations as a preliminary roadmap during assembly planning.
Table 1: Static force (force vs distance) - interaction chart
MP 62x42x25 / N38
| Distance (mm) | Induction (Gauss) / mT | Pull Force (kg/lbs/g/N) | Risk Status |
|---|---|---|---|
| 0 mm |
3891 Gs
389.1 mT
|
58.67 kg / 129.35 pounds
58670.0 g / 575.6 N
|
dangerous! |
| 1 mm |
3784 Gs
378.4 mT
|
55.50 kg / 122.35 pounds
55496.2 g / 544.4 N
|
dangerous! |
| 2 mm |
3673 Gs
367.3 mT
|
52.28 kg / 115.25 pounds
52276.1 g / 512.8 N
|
dangerous! |
| 3 mm |
3559 Gs
355.9 mT
|
49.07 kg / 108.19 pounds
49072.9 g / 481.4 N
|
dangerous! |
| 5 mm |
3324 Gs
332.4 mT
|
42.83 kg / 94.42 pounds
42826.3 g / 420.1 N
|
dangerous! |
| 10 mm |
2738 Gs
273.8 mT
|
29.05 kg / 64.04 pounds
29047.2 g / 285.0 N
|
dangerous! |
| 15 mm |
2200 Gs
220.0 mT
|
18.76 kg / 41.35 pounds
18757.5 g / 184.0 N
|
dangerous! |
| 20 mm |
1745 Gs
174.5 mT
|
11.79 kg / 26.00 pounds
11794.1 g / 115.7 N
|
dangerous! |
| 30 mm |
1090 Gs
109.0 mT
|
4.60 kg / 10.14 pounds
4600.1 g / 45.1 N
|
medium risk |
| 50 mm |
460 Gs
46.0 mT
|
0.82 kg / 1.81 pounds
821.6 g / 8.1 N
|
low risk |
Table 2: Sliding capacity (wall)
MP 62x42x25 / N38
| Distance (mm) | Friction coefficient | Pull Force (kg/lbs/g/N) |
|---|---|---|
| 0 mm | Raw steel (µ ≈ 0.2) |
11.73 kg / 25.87 pounds
11734.0 g / 115.1 N
|
| 1 mm | Raw steel (µ ≈ 0.2) |
11.10 kg / 24.47 pounds
11100.0 g / 108.9 N
|
| 2 mm | Raw steel (µ ≈ 0.2) |
10.46 kg / 23.05 pounds
10456.0 g / 102.6 N
|
| 3 mm | Raw steel (µ ≈ 0.2) |
9.81 kg / 21.64 pounds
9814.0 g / 96.3 N
|
| 5 mm | Raw steel (µ ≈ 0.2) |
8.57 kg / 18.88 pounds
8566.0 g / 84.0 N
|
| 10 mm | Raw steel (µ ≈ 0.2) |
5.81 kg / 12.81 pounds
5810.0 g / 57.0 N
|
| 15 mm | Raw steel (µ ≈ 0.2) |
3.75 kg / 8.27 pounds
3752.0 g / 36.8 N
|
| 20 mm | Raw steel (µ ≈ 0.2) |
2.36 kg / 5.20 pounds
2358.0 g / 23.1 N
|
| 30 mm | Raw steel (µ ≈ 0.2) |
0.92 kg / 2.03 pounds
920.0 g / 9.0 N
|
| 50 mm | Raw steel (µ ≈ 0.2) |
0.16 kg / 0.36 pounds
164.0 g / 1.6 N
|
Table 3: Vertical assembly (sliding) - behavior on slippery surfaces
MP 62x42x25 / N38
| Surface type | Friction coefficient / % | Max load (kg/lbs/g/N) |
|---|---|---|
| Raw steel |
µ = 0.3
30% of nominal force
|
17.60 kg / 38.80 pounds
17601.0 g / 172.7 N
|
| Painted steel (standard) |
µ = 0.2
20% of nominal force
|
11.73 kg / 25.87 pounds
11734.0 g / 115.1 N
|
| Oily/slippery steel |
µ = 0.1
10% of nominal force
|
5.87 kg / 12.93 pounds
5867.0 g / 57.6 N
|
| Magnet with anti-slip rubber |
µ = 0.5
50% of nominal force
|
29.34 kg / 64.67 pounds
29335.0 g / 287.8 N
|
Table 4: Steel thickness (saturation) - sheet metal selection
MP 62x42x25 / N38
| Steel thickness (mm) | % power | Real pull force (kg/lbs/g/N) |
|---|---|---|
| 0.5 mm |
|
1.96 kg / 4.31 pounds
1955.7 g / 19.2 N
|
| 1 mm |
|
4.89 kg / 10.78 pounds
4889.2 g / 48.0 N
|
| 2 mm |
|
9.78 kg / 21.56 pounds
9778.3 g / 95.9 N
|
| 3 mm |
|
14.67 kg / 32.34 pounds
14667.5 g / 143.9 N
|
| 5 mm |
|
24.45 kg / 53.89 pounds
24445.8 g / 239.8 N
|
| 10 mm |
|
48.89 kg / 107.79 pounds
48891.7 g / 479.6 N
|
| 11 mm |
|
53.78 kg / 118.57 pounds
53780.8 g / 527.6 N
|
| 12 mm |
|
58.67 kg / 129.35 pounds
58670.0 g / 575.6 N
|
Table 5: Thermal stability (stability) - thermal limit
MP 62x42x25 / N38
| Magnet temperature (°C) | Force change relative to 20°C | Remaining pull (kg/lbs/g/N) | Status |
|---|---|---|---|
| 20 °C | 0.0% |
58.67 kg / 129.35 pounds
58670.0 g / 575.6 N
|
Estimate |
| 40 °C | -4.4% |
56.12 kg / 123.72 pounds
56116.9 g / 550.5 N
|
Estimate |
| 60 °C | -8.6% |
53.62 kg / 118.21 pounds
53620.6 g / 526.0 N
|
Estimate |
| 80 °C | -12.8% |
51.18 kg / 112.83 pounds
51181.1 g / 502.1 N
|
Material limit |
| 100 °C | — | — | Out of range — no model |
Table 6: Two magnets (attraction) - field range
MP 62x42x25 / N38
| Gap (mm) | Attraction (kg/lbs) (N-S) | Shear Force (kg/lbs/g/N) | Repulsion (kg/lbs) (N-N) |
|---|---|---|---|
| 0 mm |
152.48 kg / 336.16 pounds
5 268 Gs
|
22.87 kg / 50.42 pounds
22872 g / 224.4 N
|
N/A |
| 1 mm |
148.41 kg / 327.18 pounds
7 677 Gs
|
22.26 kg / 49.08 pounds
22261 g / 218.4 N
|
133.57 kg / 294.46 pounds
~0 Gs
|
| 2 mm |
144.23 kg / 317.97 pounds
7 569 Gs
|
21.63 kg / 47.70 pounds
21635 g / 212.2 N
|
129.81 kg / 286.18 pounds
~0 Gs
|
| 3 mm |
140.05 kg / 308.75 pounds
7 458 Gs
|
21.01 kg / 46.31 pounds
21007 g / 206.1 N
|
126.04 kg / 277.87 pounds
~0 Gs
|
| 5 mm |
131.69 kg / 290.33 pounds
7 232 Gs
|
19.75 kg / 43.55 pounds
19753 g / 193.8 N
|
118.52 kg / 261.29 pounds
~0 Gs
|
| 10 mm |
111.30 kg / 245.38 pounds
6 649 Gs
|
16.70 kg / 36.81 pounds
16695 g / 163.8 N
|
100.17 kg / 220.84 pounds
~0 Gs
|
| 20 mm |
75.49 kg / 166.43 pounds
5 476 Gs
|
11.32 kg / 24.96 pounds
11324 g / 111.1 N
|
67.94 kg / 149.79 pounds
~0 Gs
|
| 50 mm |
19.11 kg / 42.12 pounds
2 755 Gs
|
2.87 kg / 6.32 pounds
2866 g / 28.1 N
|
17.20 kg / 37.91 pounds
~0 Gs
|
| 60 mm |
11.96 kg / 26.36 pounds
2 179 Gs
|
1.79 kg / 3.95 pounds
1793 g / 17.6 N
|
10.76 kg / 23.72 pounds
~0 Gs
|
| 70 mm |
7.57 kg / 16.69 pounds
1 734 Gs
|
1.14 kg / 2.50 pounds
1136 g / 11.1 N
|
6.81 kg / 15.02 pounds
~0 Gs
|
| 80 mm |
4.87 kg / 10.74 pounds
1 391 Gs
|
0.73 kg / 1.61 pounds
731 g / 7.2 N
|
4.39 kg / 9.67 pounds
~0 Gs
|
| 90 mm |
3.19 kg / 7.04 pounds
1 126 Gs
|
0.48 kg / 1.06 pounds
479 g / 4.7 N
|
2.88 kg / 6.34 pounds
~0 Gs
|
| 100 mm |
2.14 kg / 4.71 pounds
921 Gs
|
0.32 kg / 0.71 pounds
320 g / 3.1 N
|
1.92 kg / 4.24 pounds
~0 Gs
|
Table 7: Axial field levels — not safety zones
MP 62x42x25 / N38
| Field level (Gs) | mT | Model distance (cm) |
|---|---|---|
| < 5 Gs | < 0.5 mT | 30.0 cm |
| < 10 Gs | < 1.0 mT | 23.5 cm |
| < 20 Gs | < 2.0 mT | 18.5 cm |
| < 40 Gs | < 4.0 mT | 14.5 cm |
| < 50 Gs | < 5.0 mT | 13.0 cm |
| < 400 Gs | < 40.0 mT | 5.5 cm |
| < 600 Gs | < 60.0 mT | 4.5 cm |
Table 8: Collisions (kinetic energy) - collision effects
MP 62x42x25 / N38
| Start from (mm) | Speed (km/h) | Energy (J) | Predicted outcome |
|---|---|---|---|
| 10 mm |
18.93 km/h
(5.26 m/s)
|
4.24 J | |
| 30 mm |
24.13 km/h
(6.70 m/s)
|
6.88 J | |
| 50 mm |
24.86 km/h
(6.90 m/s)
|
7.30 J | |
| 100 mm |
25.04 km/h
(6.96 m/s)
|
7.41 J |
Table 9: Coating parameters (durability)
MP 62x42x25 / N38
| Technical parameter | Value / Description |
|---|---|
| Coating type | [NiCuNi] Nickel |
| Layer structure | Nickel - Copper - Nickel |
| Layer thickness | 10-20 µm |
| Salt spray test (SST) ? | 24 h |
| Recommended environment | Indoors only (dry) |
Table 10: Electrical data (Pc)
MP 62x42x25 / N38
| Parameter | Value | SI Unit / Description |
|---|---|---|
| Magnetic Flux | 75 511 Mx | 755.1 µWb |
| Pc Coefficient | 0.62 | High (Stable) |
Table 11: Underwater work (magnet fishing)
MP 62x42x25 / N38
| Environment | Effective steel pull | Effect |
|---|---|---|
| Air (land) | 58.67 kg | Standard |
| Water (riverbed) |
67.18 kg
(+8.51 kg buoyancy gain)
|
+14.5% |
1. Vertical hold
*Note: On a vertical wall, the magnet retains only a fraction of its nominal pull.
2. Steel saturation
*Thin steel (e.g. 0.5mm PC case) significantly weakens the holding force.
3. Power loss vs temp
N38: the maximum material working temperature is 80°C. Permitted conditions also depend on the shape and magnetic circuit.
4. Demagnetization curve and operating point (B-H)
chart generated for the permeance coefficient Pc (Permeance Coefficient) = 0.62
This simulation demonstrates the magnetic stability of the selected magnet under specific geometric conditions. The solid red line represents the demagnetization curve (material potential), while the dashed blue line is the load line based on the magnet's geometry. The Pc (Permeance Coefficient), also known as the load line slope, is a dimensionless value that describes the relationship between the magnet's shape and its magnetic stability. The intersection of these two lines (the black dot) is the operating point — it determines the actual magnetic flux density generated by the magnet in this specific configuration. A higher Pc value means the magnet is more 'slender' (tall relative to its area), resulting in a higher operating point and better resistance to irreversible demagnetization caused by external fields or temperature. At low Pc values (typical for flat magnets, below about 1) the operating point is closer to the 'knee' of the curve — caution is advised when operating at temperatures near the maximum limit to avoid strength loss.
Elemental analysis
| iron (Fe) | 64% – 68% |
| neodymium (Nd) | 29% – 32% |
| boron (B) | 1.1% – 1.2% |
| dysprosium (Dy) | 0.5% – 2.0% |
| coating (Ni-Cu-Ni) | < 0.05% |
Ecology and recycling (GPSR)
| recyclability (EoL) | 100% |
| recycled raw materials | ~10% (pre-cons) |
| carbon footprint | low / zredukowany |
| waste code (EWC) | 16 02 16 |
Other offers
Strengths and weaknesses of Nd2Fe14B magnets.
Advantages
- They do not lose magnetism, even over approximately ten years – the reduction in strength is only ~1% (according to tests),
- They show high resistance to demagnetization induced by external magnetic fields,
- Thanks to the glossy finish, the plating of nickel, gold, or silver gives an professional appearance,
- They are known for high magnetic induction at the operating surface, making them more effective,
- Thanks to resistance to high temperature, they can operate (depending on the shape) even at temperatures up to 230°C and higher...
- Thanks to freedom in shaping and the capacity to adapt to complex applications,
- Wide application in advanced technology sectors – they serve a role in computer drives, drive modules, medical devices, also technologically advanced constructions.
- Thanks to their power density, small magnets offer high operating force, in miniature format,
Limitations
- To avoid cracks under impact, we recommend using special steel holders. Such a solution protects the magnet and simultaneously improves its durability.
- Do not exceed this material temperature limit: 80°C. Overheating may permanently weaken the magnet.
- They oxidize in a humid environment. For use outdoors we recommend using waterproof magnets e.g. in rubber, plastic
- Limited ability of producing threads in the magnet and complicated shapes - preferred is cover - mounting mechanism.
- Potential hazard resulting from small fragments of magnets pose a threat, if swallowed, which is particularly important in the context of child safety. It is also worth noting that small components of these devices can disrupt the diagnostic process medical in case of swallowing.
- With mass production the cost of neodymium magnets is a challenge,
Pull force analysis
Maximum lifting capacity of the magnet – what affects it?
- with the application of a yoke made of low-carbon steel, guaranteeing maximum field concentration
- whose transverse dimension reaches at least 10 mm
- with an polished contact surface
- with zero gap (without impurities)
- under axial force direction (90-degree angle)
- at temperature approx. 20 degrees Celsius
Key elements affecting lifting force
- Distance (betwixt the magnet and the metal), because even a microscopic distance (e.g. 0.5 mm) can cause a reduction in lifting capacity by up to 50% (this also applies to paint, corrosion or debris).
- Loading method – catalog parameter refers to pulling vertically. When applying parallel force, the magnet exhibits much less (typically approx. 20-30% of nominal force).
- Element thickness – to utilize 100% power, the steel must be adequately massive. Thin sheet restricts the attraction force (the magnet "punches through" it).
- Material composition – different alloys reacts the same. Alloy additives worsen the attraction effect.
- Plate texture – smooth surfaces guarantee perfect abutment, which improves field saturation. Rough surfaces reduce efficiency.
- Operating temperature – NdFeB sinters have a negative temperature coefficient. At higher temperatures they are weaker, and at low temperatures gain strength (up to a certain limit).
Holding force was tested on a smooth steel plate of 20 mm thickness, when a perpendicular force was applied, however under shearing force the lifting capacity is smaller. Moreover, even a slight gap between the magnet and the plate decreases the lifting capacity.
H&S for magnets
Heat warning
Do not exceed the maximum operating temperature stated in the specifications of the particular product. The limit depends on the material, geometry and operating arrangement; there is no single threshold for all neodymium magnets. Overheating can permanently weaken a magnet.
No play value
Strictly keep magnets away from children. Risk of swallowing is high, and the effects of magnets connecting inside the body are tragic.
Life threat
Life threat: Neodymium magnets can deactivate heart devices and defibrillators. Stay away if you have electronic implants.
Respect the power
Use magnets consciously. Their powerful strength can shock even professionals. Be vigilant and do not underestimate their power.
Dust is flammable
Mechanical processing of NdFeB material poses a fire risk. Neodymium dust oxidizes rapidly with oxygen and is difficult to extinguish.
Shattering risk
Protect your eyes. Magnets can fracture upon violent connection, ejecting sharp fragments into the air. Wear goggles.
Safe distance
Do not bring magnets near a purse, laptop, or TV. The magnetism can permanently damage these devices and wipe information from cards.
GPS Danger
A powerful magnetic field interferes with the functioning of compasses in phones and GPS navigation. Do not bring magnets near a device to prevent breaking the sensors.
Avoid contact if allergic
Certain individuals have a contact allergy to nickel, which is the common plating for NdFeB magnets. Extended handling might lead to an allergic reaction. It is best to use protective gloves.
Pinching danger
Watch your fingers. Two powerful magnets will join immediately with a force of massive weight, crushing anything in their path. Be careful!
