MW 3x2 zestaw 100 szt. / N38 - cylindrical magnet
cylindrical magnet
Catalog no 010539
GTIN/EAN: 5906301815303
- Diameter Ø
- 3 mm [±0,1 mm]
- Height
- 2 mm [±0,1 mm]
- Weight
- 11 g
- Magnetization Direction
- ↑ axial
- Coating
- [NiCuNi] Nickel
How we measure these parameters — certificates and measurements
16.25 zł net / pcs
19.99 zł with VAT (23% VAT) / pcs
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Need more?Frequently asked questions
Where can I buy strong cylindrical neodymium magnets?
Can a small cylindrical magnet provide a strong grip for precise workshop work?
Which cylindrical magnet can work at a higher temperature?
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 - MW 3x2 zestaw 100 szt. / N38 - cylindrical magnet
Specification / characteristics - MW 3x2 zestaw 100 szt. / N38 - cylindrical magnet
| properties | values |
|---|---|
| Cat. no. | 010539 |
| GTIN/EAN | 5906301815303 |
| Distributor | Dhit sp. z o.o. |
| Country of origin | Poland / China / Germany |
| Customs code | 85059029 |
| Diameter Ø | 3 mm [±0,1 mm] |
| Height | 2 mm [±0,1 mm] |
| Weight | 11 g |
| Magnetization Direction | ↑ axial |
| Load capacity ~ ? | 0.30 kg / 2.99 N |
| Magnetic Induction ~ ? | 493.99 mT / 4940 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 |
Physical simulation of the magnet - data
These information are the outcome of a engineering analysis. Results are based on models for the class Nd2Fe14B. Actual conditions may deviate from the simulation results. Use these data as a preliminary roadmap during assembly planning.
Table 1: Static pull force (force vs gap) - power drop
MW 3x2 zestaw 100 szt. / N38
| Distance (mm) | Induction (Gauss) / mT | Pull Force (kg/lbs/g/N) | Risk Status |
|---|---|---|---|
| 0 mm |
4928 Gs
492.8 mT
|
0.30 kg / 0.66 lbs
300.0 g / 2.9 N
|
weak grip |
| 1 mm |
2106 Gs
210.6 mT
|
0.05 kg / 0.12 lbs
54.8 g / 0.5 N
|
weak grip |
| 2 mm |
845 Gs
84.5 mT
|
0.01 kg / 0.02 lbs
8.8 g / 0.1 N
|
weak grip |
| 3 mm |
393 Gs
39.3 mT
|
0.00 kg / 0.00 lbs
1.9 g / 0.0 N
|
weak grip |
| 5 mm |
124 Gs
12.4 mT
|
0.00 kg / 0.00 lbs
0.2 g / 0.0 N
|
weak grip |
| 10 mm |
21 Gs
2.1 mT
|
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
weak grip |
| 15 mm |
7 Gs
0.7 mT
|
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
weak grip |
| 20 mm |
3 Gs
0.3 mT
|
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
weak grip |
| 30 mm |
1 Gs
0.1 mT
|
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
weak grip |
| 50 mm |
0 Gs
0.0 mT
|
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
weak grip |
Table 2: Slippage load (vertical surface)
MW 3x2 zestaw 100 szt. / N38
| Distance (mm) | Friction coefficient | Pull Force (kg/lbs/g/N) |
|---|---|---|
| 0 mm | Raw steel (µ ≈ 0.2) |
0.06 kg / 0.13 lbs
60.0 g / 0.6 N
|
| 1 mm | Raw steel (µ ≈ 0.2) |
0.01 kg / 0.02 lbs
10.0 g / 0.1 N
|
| 2 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 lbs
2.0 g / 0.0 N
|
| 3 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
| 5 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
| 10 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
| 15 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
| 20 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
| 30 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
| 50 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
Table 3: Wall mounting (shearing) - behavior on slippery surfaces
MW 3x2 zestaw 100 szt. / N38
| Surface type | Friction coefficient / % | Max load (kg/lbs/g/N) |
|---|---|---|
| Raw steel |
µ = 0.3
30% of nominal force
|
0.09 kg / 0.20 lbs
90.0 g / 0.9 N
|
| Painted steel (standard) |
µ = 0.2
20% of nominal force
|
0.06 kg / 0.13 lbs
60.0 g / 0.6 N
|
| Oily/slippery steel |
µ = 0.1
10% of nominal force
|
0.03 kg / 0.07 lbs
30.0 g / 0.3 N
|
| Magnet with anti-slip rubber |
µ = 0.5
50% of nominal force
|
0.15 kg / 0.33 lbs
150.0 g / 1.5 N
|
Table 4: Steel thickness (substrate influence) - power losses
MW 3x2 zestaw 100 szt. / N38
| Steel thickness (mm) | % power | Real pull force (kg/lbs/g/N) |
|---|---|---|
| 0.5 mm |
|
0.03 kg / 0.07 lbs
30.0 g / 0.3 N
|
| 1 mm |
|
0.08 kg / 0.17 lbs
75.0 g / 0.7 N
|
| 2 mm |
|
0.15 kg / 0.33 lbs
150.0 g / 1.5 N
|
| 3 mm |
|
0.22 kg / 0.50 lbs
225.0 g / 2.2 N
|
| 5 mm |
|
0.30 kg / 0.66 lbs
300.0 g / 2.9 N
|
| 10 mm |
|
0.30 kg / 0.66 lbs
300.0 g / 2.9 N
|
| 11 mm |
|
0.30 kg / 0.66 lbs
300.0 g / 2.9 N
|
| 12 mm |
|
0.30 kg / 0.66 lbs
300.0 g / 2.9 N
|
Table 5: Working in heat (material behavior) - thermal limit
MW 3x2 zestaw 100 szt. / N38
| Magnet temperature (°C) | Force change relative to 20°C | Remaining pull (kg/lbs/g/N) | Status |
|---|---|---|---|
| 20 °C | 0.0% |
0.30 kg / 0.66 lbs
300.0 g / 2.9 N
|
Estimate |
| 40 °C | -4.4% |
0.29 kg / 0.63 lbs
286.9 g / 2.8 N
|
Estimate |
| 60 °C | -8.6% |
0.27 kg / 0.60 lbs
274.2 g / 2.7 N
|
Estimate |
| 80 °C | -12.8% |
0.26 kg / 0.58 lbs
261.7 g / 2.6 N
|
Material limit |
| 100 °C | — | — | Out of range — no model |
Table 6: Magnet-Magnet interaction (repulsion) - field range
MW 3x2 zestaw 100 szt. / N38
| Gap (mm) | Attraction (kg/lbs) (N-S) | Shear Strength (kg/lbs/g/N) | Repulsion (kg/lbs) (N-N) |
|---|---|---|---|
| 0 mm |
1.06 kg / 2.33 lbs
5 766 Gs
|
0.16 kg / 0.35 lbs
159 g / 1.6 N
|
N/A |
| 1 mm |
0.49 kg / 1.08 lbs
6 712 Gs
|
0.07 kg / 0.16 lbs
74 g / 0.7 N
|
0.44 kg / 0.97 lbs
~0 Gs
|
| 2 mm |
0.19 kg / 0.43 lbs
4 213 Gs
|
0.03 kg / 0.06 lbs
29 g / 0.3 N
|
0.17 kg / 0.38 lbs
~0 Gs
|
| 3 mm |
0.08 kg / 0.17 lbs
2 629 Gs
|
0.01 kg / 0.02 lbs
11 g / 0.1 N
|
0.07 kg / 0.15 lbs
~0 Gs
|
| 5 mm |
0.01 kg / 0.03 lbs
1 131 Gs
|
0.00 kg / 0.00 lbs
2 g / 0.0 N
|
0.01 kg / 0.03 lbs
~0 Gs
|
| 10 mm |
0.00 kg / 0.00 lbs
248 Gs
|
0.00 kg / 0.00 lbs
0 g / 0.0 N
|
0.00 kg / 0.00 lbs
~0 Gs
|
| 20 mm |
0.00 kg / 0.00 lbs
41 Gs
|
0.00 kg / 0.00 lbs
0 g / 0.0 N
|
0.00 kg / 0.00 lbs
~0 Gs
|
| 50 mm |
0.00 kg / 0.00 lbs
3 Gs
|
0.00 kg / 0.00 lbs
0 g / 0.0 N
|
0.00 kg / 0.00 lbs
~0 Gs
|
| 60 mm |
0.00 kg / 0.00 lbs
2 Gs
|
0.00 kg / 0.00 lbs
0 g / 0.0 N
|
0.00 kg / 0.00 lbs
~0 Gs
|
| 70 mm |
0.00 kg / 0.00 lbs
1 Gs
|
0.00 kg / 0.00 lbs
0 g / 0.0 N
|
0.00 kg / 0.00 lbs
~0 Gs
|
| 80 mm |
0.00 kg / 0.00 lbs
1 Gs
|
0.00 kg / 0.00 lbs
0 g / 0.0 N
|
0.00 kg / 0.00 lbs
~0 Gs
|
| 90 mm |
0.00 kg / 0.00 lbs
1 Gs
|
0.00 kg / 0.00 lbs
0 g / 0.0 N
|
0.00 kg / 0.00 lbs
~0 Gs
|
| 100 mm |
0.00 kg / 0.00 lbs
0 Gs
|
0.00 kg / 0.00 lbs
0 g / 0.0 N
|
0.00 kg / 0.00 lbs
~0 Gs
|
Table 7: Axial field levels — not safety zones
MW 3x2 zestaw 100 szt. / N38
| Field level (Gs) | mT | Model distance (cm) |
|---|---|---|
| < 5 Gs | < 0.5 mT | 2.0 cm |
| < 10 Gs | < 1.0 mT | 1.5 cm |
| < 20 Gs | < 2.0 mT | 1.5 cm |
| < 40 Gs | < 4.0 mT | 1.0 cm |
| < 50 Gs | < 5.0 mT | 1.0 cm |
| < 400 Gs | < 40.0 mT | 0.5 cm |
| < 600 Gs | < 60.0 mT | 0.5 cm |
Table 8: Dynamics (cracking risk) - collision effects
MW 3x2 zestaw 100 szt. / N38
| Start from (mm) | Speed (km/h) | Energy (J) | Predicted outcome |
|---|---|---|---|
| 10 mm |
2.06 km/h
(0.57 m/s)
|
0.00 J | |
| 30 mm |
2.06 km/h
(0.57 m/s)
|
0.00 J | |
| 50 mm |
2.06 km/h
(0.57 m/s)
|
0.00 J | |
| 100 mm |
2.06 km/h
(0.57 m/s)
|
0.00 J |
Table 9: Surface protection spec
MW 3x2 zestaw 100 szt. / 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: Construction data (Flux)
MW 3x2 zestaw 100 szt. / N38
| Parameter | Value | SI Unit / Description |
|---|---|---|
| Magnetic Flux | 353 Mx | 3.5 µWb |
| Pc Coefficient | 0.71 | High (Stable) |
Table 11: Submerged application
MW 3x2 zestaw 100 szt. / N38
| Environment | Effective steel pull | Effect |
|---|---|---|
| Air (land) | 0.30 kg | Standard |
| Water (riverbed) |
0.34 kg
(+0.04 kg buoyancy gain)
|
+14.5% |
1. Shear force
*Note: On a vertical surface, the magnet retains merely a fraction of its perpendicular strength.
2. Plate thickness effect
*Thin metal sheet (e.g. computer case) severely weakens the holding force.
3. Thermal stability
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) = 0.71
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. A value of 0.42 is relatively low (typical for flat magnets), meaning 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.
Chemical composition
| 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% |
Sustainability
| recyclability (EoL) | 100% |
| recycled raw materials | ~10% (pre-cons) |
| carbon footprint | low / zredukowany |
| waste code (EWC) | 16 02 16 |
Other deals
Strengths and weaknesses of neodymium magnets.
Strengths
- They have constant strength, and over around 10 years their performance decreases symbolically – ~1% (in testing),
- They retain their magnetic properties even under close interference source,
- Thanks to the shimmering finish, the surface of nickel, gold, or silver gives an clean appearance,
- Magnets exhibit excellent magnetic induction on the outer side,
- Thanks to resistance to high temperature, they are able to function (depending on the shape) even at temperatures up to 230°C and higher...
- Due to the potential of accurate molding and adaptation to custom solutions, neodymium magnets can be produced in a broad palette of forms and dimensions, which makes them more universal,
- Universal use in modern industrial fields – they are used in HDD drives, drive modules, medical equipment, also modern systems.
- Thanks to their power density, small magnets offer high operating force, in miniature format,
Disadvantages
- Susceptibility to cracking is one of their disadvantages. Upon strong impact they can fracture. We recommend keeping them in a steel housing, which not only protects them against impacts but also increases their durability
- Do not exceed this material temperature limit: 80°C. Overheating may permanently weaken the magnet.
- Magnets exposed to a humid environment can corrode. Therefore when using outdoors, we recommend using waterproof magnets made of rubber, plastic or other material resistant to moisture
- Due to limitations in producing threads and complicated shapes in magnets, we recommend using casing - magnetic mechanism.
- Possible danger related to microscopic parts of magnets can be dangerous, if swallowed, which gains importance in the context of child health protection. Furthermore, small components of these devices can be problematic in diagnostics medical when they are in the body.
- Due to expensive raw materials, their price is relatively high,
Lifting parameters
Maximum magnetic pulling force – what affects it?
- on a plate made of structural steel, optimally conducting the magnetic field
- possessing a massiveness of at least 10 mm to ensure full flux closure
- characterized by even structure
- under conditions of ideal adhesion (metal-to-metal)
- under vertical force direction (90-degree angle)
- at room temperature
Lifting capacity in real conditions – factors
- Gap between magnet and steel – every millimeter of distance (caused e.g. by varnish or unevenness) significantly weakens the magnet efficiency, often by half at just 0.5 mm.
- Loading method – declared lifting capacity refers to pulling vertically. When slipping, the magnet holds significantly lower power (typically approx. 20-30% of maximum force).
- Plate thickness – insufficiently thick steel causes magnetic saturation, causing part of the flux to be wasted into the air.
- Steel type – mild steel attracts best. Alloy admixtures lower magnetic properties and lifting capacity.
- Surface quality – the more even the plate, the better the adhesion and higher the lifting capacity. Unevenness acts like micro-gaps.
- Heat – neodymium magnets have a sensitivity to temperature. At higher temperatures they lose power, and at low temperatures they can be stronger (up to a certain limit).
Lifting capacity testing was conducted on plates with a smooth surface of suitable thickness, under perpendicular forces, however under attempts to slide the magnet the load capacity is reduced by as much as 5 times. Moreover, even a slight gap between the magnet and the plate lowers the load capacity.
Precautions when working with neodymium magnets
Handling rules
Before use, read the rules. Uncontrolled attraction can break the magnet or hurt your hand. Be predictive.
Serious injuries
Large magnets can smash fingers instantly. Do not place your hand between two strong magnets.
Product not for children
These products are not toys. Swallowing a few magnets can lead to them attracting across intestines, which constitutes a direct threat to life and requires immediate surgery.
Protective goggles
Watch out for shards. Magnets can explode upon uncontrolled impact, ejecting shards into the air. Eye protection is mandatory.
Electronic hazard
Avoid bringing magnets close to a wallet, laptop, or TV. The magnetism can irreversibly ruin these devices and erase data from cards.
Magnetic interference
GPS units and mobile phones are highly susceptible to magnetic fields. Direct contact with a powerful NdFeB magnet can ruin the internal compass in your phone.
Allergic reactions
Nickel alert: The nickel-copper-nickel coating contains nickel. If skin irritation occurs, cease working with magnets and use protective gear.
Dust explosion hazard
Powder generated during cutting of magnets is flammable. Do not drill into magnets without proper cooling and knowledge.
Permanent damage
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.
Warning for heart patients
Medical warning: Strong magnets can deactivate pacemakers and defibrillators. Do not approach if you have electronic implants.
